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"phyloDocs": "714.0", "phyloFoundations": "484", "phyloGroups": "440", "phyloPeriods": "51", "phyloQuality": "0.5022782592937735", "phyloSeaRiseStart": "0.1", "phyloSeaRiseSteps": "0.1", "phyloSources": "[]", "phyloTerms": "436", "phyloTimeScale": "year", "rank": "same", "ranksep": "1", "ratio": "fill", "splines": "spline", "style": "filled", "_gvid": 50, "nodes": [ 536,537,538,539,540,541,542,543 ] }, { "name": "Period20202022", "PhyloScale": "0.77", "bb": "0,0,33444,54969", "color": "white", "fontsize": "30", "label": "parisi_v3", "labelloc": "t", "lheight": "0.46", "lp": "16722,54948", "lwidth": "1.93", "nodesep": "1", "overlap": "scale", "phyloBranches": "6", "phyloDocs": "714.0", "phyloFoundations": "484", "phyloGroups": "440", "phyloPeriods": "51", "phyloQuality": "0.5022782592937735", "phyloSeaRiseStart": "0.1", "phyloSeaRiseSteps": "0.1", "phyloSources": "[]", "phyloTerms": "436", "phyloTimeScale": "year", "rank": "same", "ranksep": "1", "ratio": "fill", "splines": "spline", "style": "filled", "_gvid": 51, "nodes": [ 544,545,546,547,548 ] }, { "_gvid": 52, "name": "branch[0,14,1,1,1]", "age": "10.0", "bId": "0", "birth": "1970.0", "branchId": "0 14 1 1 1", "branch_x": "10.899999999999999", "branch_y": "0.0", "fillcolor": "cornsilk", "fontname": "Arial", "fontsize": "40", "height": "1.0217", "label": "\"expansion | quantum field theory\"", "nodeType": "branch", "pos": "2722.5,54891", "shape": "egg", "size": "4.0", "style": "bold", "width": "13.157" }, { "_gvid": 53, "name": "branch[0,33,1,1,1,1,1,1]", "age": "9.0", "bId": "1", "birth": "1975.0", "branchId": "0 33 1 1 1 1 1 1", "branch_x": "37.70000000000001", "branch_y": "0.0", "fillcolor": "cornsilk", "fontname": "Arial", "fontsize": "40", "height": "1.0217", "label": "\"asymptotic estimates | higgs boson mass\"", "nodeType": "branch", "pos": "4637.5,54891", "shape": "egg", "size": "4.0", "style": "bold", "width": "16.316" }, { "_gvid": 54, "name": "branch[0,45,1,1,1,1]", "age": "4.0", "bId": "2", "birth": "1986.0", "branchId": "0 45 1 1 1 1", "branch_x": "55.40000000000001", "branch_y": "0.0", "fillcolor": "cornsilk", "fontname": "Arial", "fontsize": "40", "height": "1.0217", "label": "\"ape computer | lattice size\"", "nodeType": "branch", "pos": "5926.5,54891", "shape": "egg", "size": "3.0", "style": "bold", "width": "10.752" }, { "_gvid": 55, "name": "branch[0,46,1,1,1,1,1,1,1]", "age": "6.0", "bId": "3", "birth": "1987.0", "branchId": "0 46 1 1 1 1 1 1 1", "branch_x": "56.70000000000001", "branch_y": "0.0", "fillcolor": "cornsilk", "fontname": "Arial", "fontsize": "40", "height": "1.0217", "label": "\"memory capacity | informa uk ltd all rights\"", "nodeType": "branch", "pos": "7929.5,54891", "shape": "egg", "size": "3.0", "style": "bold", "width": "16.462" }, { "_gvid": 56, "name": "branch[0,71,1,24]", "age": "48.0", "bId": "4", "birth": "1974.0", "branchId": "0 71 1 24", "branch_x": "81.09999999999997", "branch_y": "0.0", "fillcolor": "cornsilk", "fontname": "Arial", "fontsize": "40", "height": "1.0217", "label": "\"spin glasses | scaling\"", "nodeType": "branch", "pos": "24116,54891", "shape": "egg", "size": "45.0", "style": "bold", "width": "8.9317" }, { "_gvid": 57, "name": "branch[0,71,1,12,1]", "age": "6.0", "bId": "5", "birth": "2006.0", "branchId": "0 71 1 12 1", "branch_x": "96.29999999999997", "branch_y": "0.2", "fillcolor": "cornsilk", "fontname": "Arial", "fontsize": "40", "height": "1.0217", "label": "\"neighbours | large flocks\"", "nodeType": "branch", "pos": "31826,54891", "shape": "egg", "size": "4.0", "style": "bold", "width": "10.103" }, { "_gvid": 58, "name": "period19701972", "fontsize": "50", "from": "1970", "height": "0.875", "label": "1970 1972", "nodeType": "period", "pos": "33302,54352", "shape": "box", "strFrom": "\"1970-10-09\"", "strTo": "\"1972-10-09\"", "to": "1972", "width": "3.9444" }, { "_gvid": 59, "name": "group1970197220", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"2 | 4 | 24 | 25\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "1970", "gid": "group1970197220", "height": "11.931", "label": "
PERTURBATION THEORY | CONFORMAL INVARIANCE ( 1970 , 1972 ) (((1970,1972),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
perturbation theory<\/TD> conformal invariance<\/TD> scaling<\/TD> ward identities<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ward identities | scaling | conformal invariance | perturbation theory\"", "nodeType": "group", "penwidth": "4", "pos": "1482.5,54352", "role": "\"0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1970-10-09\"", "strTo": "\"1972-10-09\"", "support": "1", "to": "1972", "weight": "Just 1.0", "width": "11.931" }, { "_gvid": 60, "name": "group1970197221", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"4 | 12 | 13 | 14\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1970", "gid": "group1970197221", "height": "9.9167", "label": "
STRUCTURE FUNCTION | SCALING ( 1970 , 1972 ) (((1970,1972),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
structure function<\/TD> scaling<\/TD> asymptotic behaviour<\/TD> expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | asymptotic behaviour | structure function | expansion\"", "nodeType": "group", "penwidth": "4", "pos": "3901.5,54352", "role": "\"0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1970-10-09\"", "strTo": "\"1972-10-09\"", "support": "1", "to": "1972", "weight": "Just 1.0", "width": "9.9167" }, { "_gvid": 61, "name": "group1970197222", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"4 | 16 | 17\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1970", "gid": "group1970197222", "height": "9.6806", "label": "
QUANTUM FIELD THEORY | RENORMALIZATION ( 1970 , 1972 ) (((1970,1972),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quantum field theory<\/TD> renormalization<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | renormalization | quantum field theory\"", "nodeType": "group", "penwidth": "4", "pos": "2332.5,54352", "role": "\"0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1970-10-09\"", "strTo": "\"1972-10-09\"", "support": "1", "to": "1972", "weight": "Just 1.0", "width": "9.6806" }, { "_gvid": 62, "name": "group1970197223", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"4 | 24 | 26\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1970", "gid": "group1970197223", "height": "9.9861", "label": "
INFINITE NUMBER | CONFORMAL INVARIANCE ( 1970 , 1972 ) (((1970,1972),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
infinite number<\/TD> conformal invariance<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | conformal invariance | infinite number\"", "nodeType": "group", "penwidth": "4", "pos": "3112.5,54352", "role": "\"0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1970-10-09\"", "strTo": "\"1972-10-09\"", "support": "1", "to": "1972", "weight": "Just 1.0", "width": "9.9861" }, { "_gvid": 63, "name": "period19711973", "fontsize": "50", "from": "1971", "height": "0.875", "label": "1971 1973", "nodeType": "period", "pos": "33302,53384", "shape": "box", "strFrom": "\"1973-10-09\"", "strTo": "\"1973-10-09\"", "to": "1973", "width": "3.9444" }, { "_gvid": 64, "name": "group1971197320", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"2 | 21 | 25 | 29\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1971", "gid": "group1971197320", "height": "11.806", "label": "
PERTURBATION THEORY | WARD IDENTITIES ( 1971 , 1973 ) (((1971,1973),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
perturbation theory<\/TD> ward identities<\/TD> wilson expansion<\/TD> coupling constants<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ward identities | wilson expansion | perturbation theory | coupling constants\"", "nodeType": "group", "penwidth": "4", "pos": "846.5,53384", "role": "\"2.0 | 2.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1973-10-09\"", "strTo": "\"1973-10-09\"", "support": "1", "to": "1973", "weight": "Just 1.0", "width": "11.806" }, { "_gvid": 65, "name": "group1971197321", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"13 | 27 | 28\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1971", "gid": "group1971197321", "height": "10.736", "label": "
SCALING LAW | ANOMALOUS DIMENSIONS ( 1971 , 1973 ) (((1971,1973),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling law<\/TD> anomalous dimensions<\/TD> structure function<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"structure function | anomalous dimensions | scaling law\"", "nodeType": "group", "penwidth": "4", "pos": "2737.5,53384", "role": "\"3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1973-10-09\"", "strTo": "\"1973-10-09\"", "support": "1", "to": "1973", "weight": "Just 1.0", "width": "10.736" }, { "_gvid": 66, "name": "group1971197322", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"17 | 21 | 27 | 29\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1971", "gid": "group1971197322", "height": "12.986", "label": "
WILSON EXPANSION | COUPLING CONSTANTS ( 1971 , 1973 ) (((1971,1973),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
wilson expansion<\/TD> coupling constants<\/TD> anomalous dimensions<\/TD> quantum field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"quantum field theory | wilson expansion | anomalous dimensions | coupling constants\"", "nodeType": "group", "penwidth": "4", "pos": "1811.5,53384", "role": "\"3.0 | 2.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1973-10-09\"", "strTo": "\"1973-10-09\"", "support": "1", "to": "1973", "weight": "Just 1.0", "width": "12.986" }, { "_gvid": 67, "name": "period19721974", "fontsize": "50", "from": "1972", "height": "0.875", "label": "1972 1974", "nodeType": "period", "pos": "33302,52812", "shape": "box", "strFrom": "\"1974-10-09\"", "strTo": "\"1974-10-09\"", "to": "1974", "width": "3.9444" }, { "_gvid": 68, "name": "period19731975", "fontsize": "50", "from": "1973", "height": "0.875", "label": "1973 1975", "nodeType": "period", "pos": "33302,52312", "shape": "box", "strFrom": "\"1975-10-09\"", "strTo": "\"1975-10-09\"", "to": "1975", "width": "3.9444" }, { "_gvid": 69, "name": "group1973197521", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"16 | 17 | 29\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1973", "gid": "group1973197521", "height": "11.028", "label": "
QUANTUM FIELD THEORY | COUPLING CONSTANTS ( 1973 , 1975 ) (((1973,1975),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quantum field theory<\/TD> coupling constants<\/TD> renormalization<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization | quantum field theory | coupling constants\"", "nodeType": "group", "penwidth": "4", "pos": "3109.5,52312", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1975-10-09\"", "strTo": "\"1975-10-09\"", "support": "1", "to": "1975", "weight": "Just 1.0", "width": "11.028" }, { "_gvid": 70, "name": "period19741976", "fontsize": "50", "from": "1974", "height": "0.875", "label": "1974 1976", "nodeType": "period", "pos": "33302,51405", "shape": "box", "strFrom": "\"1976-10-09\"", "strTo": "\"1976-10-09\"", "to": "1976", "width": "3.9444" }, { "_gvid": 71, "name": "group1974197620", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"1 | 11 | 35 | 36 | 37\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1974", "gid": "group1974197620", "height": "12.167", "label": "
GROUND STATE | REGGEON FIELD THEORY ( 1974 , 1976 ) (((1974,1976),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ground state<\/TD> reggeon field theory<\/TD> phase transition<\/TD> symmetry breaking<\/TD><\/TR>\n
energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"symmetry breaking | phase transition | reggeon field theory | ground state | energy\"", "nodeType": "group", "penwidth": "4", "pos": "23880,51405", "role": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1976-10-09\"", "strTo": "\"1976-10-09\"", "support": "1", "to": "1976", "weight": "Just 1.0", "width": "12.167" }, { "_gvid": 72, "name": "group1974197621", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 37 | 38\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0\"", "from": "1974", "gid": "group1974197621", "height": "7.7917", "label": "
ASYMPTOTIC FREEDOM | ENERGY ( 1974 , 1976 ) (((1974,1976),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
asymptotic freedom<\/TD> energy<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | energy | asymptotic freedom\"", "nodeType": "group", "penwidth": "4", "pos": "24672,51405", "role": "\"1.0 | 0.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1976-10-09\"", "strTo": "\"1976-10-09\"", "support": "1", "to": "1976", "weight": "Just 1.0", "width": "7.7917" }, { "_gvid": 73, "name": "period19751977", "fontsize": "50", "from": "1975", "height": "0.875", "label": "1975 1977", "nodeType": "period", "pos": "33302,50475", "shape": "box", "strFrom": "\"1977-10-09\"", "strTo": "\"1977-10-09\"", "to": "1977", "width": "3.9444" }, { "_gvid": 74, "name": "group1975197721", "bId": "1", "branchId": "0 33 1 1 1 1 1", "fontname": "Arial", "foundation": "\"20 | 42 | 43\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1975", "gid": "group1975197721", "height": "10.5", "label": "
FEYNMAN DIAGRAM | ASYMPTOTIC ESTIMATES ( 1975 , 1977 ) (((1975,1977),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
feynman diagram<\/TD> asymptotic estimates<\/TD> high orders<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"high orders | asymptotic estimates | feynman diagram\"", "nodeType": "group", "penwidth": "4", "pos": "5409.5,50475", "role": "\"0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1977-10-09\"", "strTo": "\"1977-10-09\"", "support": "1", "to": "1977", "weight": "Just 1.0", "width": "10.5" }, { "_gvid": 75, "name": "group1975197722", "bId": "1", "branchId": "0 33 1 1 1 1 1", "fontname": "Arial", "foundation": "\"25 | 42 | 44 | 45\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1975", "gid": "group1975197722", "height": "11.667", "label": "
QUANTUM ELECTRODYNAMICS | FERMIONS ( 1975 , 1977 ) (((1975,1977),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quantum electrodynamics<\/TD> fermions<\/TD> asymptotic estimates<\/TD> perturbation theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"perturbation theory | asymptotic estimates | fermions | quantum electrodynamics\"", "nodeType": "group", "penwidth": "4", "pos": "4539.5,50475", "role": "\"1.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1977-10-09\"", "strTo": "\"1977-10-09\"", "support": "1", "to": "1977", "weight": "Just 1.0", "width": "11.667" }, { "_gvid": 76, "name": "period19761978", "fontsize": "50", "from": "1976", "height": "0.875", "label": "1976 1978", "nodeType": "period", "pos": "33302,49484", "shape": "box", "strFrom": "\"1978-10-09\"", "strTo": "\"1978-10-09\"", "to": "1978", "width": "3.9444" }, { "_gvid": 77, "name": "group1976197822", "bId": "1", "branchId": "0 33 1 1 1 1 1", "fontname": "Arial", "foundation": "\"25 | 32 | 42 | 44 | 45 | 52\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1976", "gid": "group1976197822", "height": "13.875", "label": "
EXPLICIT EXAMPLE | QUANTUM ELECTRODYNAMICS ( 1976 , 1978 ) (((1976,1978),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
explicit example<\/TD> quantum electrodynamics<\/TD> perturbation theory<\/TD> asymptotic estimates<\/TD><\/TR>\n
fermions<\/TD> perturbative expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"perturbation theory | perturbative expansion | asymptotic estimates | fermions | quantum electrodynamics | explicit example\"", "nodeType": "group", "penwidth": "4", "pos": "4539.5,49484", "role": "\"3.0 | 1.0 | 3.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1978-10-09\"", "strTo": "\"1978-10-09\"", "support": "1", "to": "1978", "weight": "Just 1.0", "width": "13.875" }, { "_gvid": 78, "name": "group1976197823", "bId": "1", "branchId": "0 33 1 1 1 1 1", "fontname": "Arial", "foundation": "\"37 | 44 | 47\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1976", "gid": "group1976197823", "height": "7.6528", "label": "
HIGGS BOSON MASS | ENERGY ( 1976 , 1978 ) (((1976,1978),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
higgs boson mass<\/TD> fermions<\/TD> energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | fermions | higgs boson mass\"", "nodeType": "group", "penwidth": "4", "pos": "3692.5,49484", "role": "\"1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1978-10-09\"", "strTo": "\"1978-10-09\"", "support": "1", "to": "1978", "weight": "Just 1.0", "width": "7.6528" }, { "_gvid": 79, "name": "period19771979", "fontsize": "50", "from": "1977", "height": "0.875", "label": "1977 1979", "nodeType": "period", "pos": "33302,48456", "shape": "box", "strFrom": "\"1979-10-09\"", "strTo": "\"1979-10-09\"", "to": "1979", "width": "3.9444" }, { "_gvid": 80, "name": "group1977197922", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"13 | 14 | 46\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1977", "gid": "group1977197922", "height": "8.4861", "label": "
QCD | STRUCTURE FUNCTION ( 1977 , 1979 ) (((1977,1979),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
qcd<\/TD> structure function<\/TD> expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"structure function | expansion | qcd\"", "nodeType": "group", "penwidth": "4", "pos": "25330,48456", "role": "\"1.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1979-10-09\"", "strTo": "\"1979-10-09\"", "support": "1", "to": "1979", "weight": "Just 1.0", "width": "8.4861" }, { "_gvid": 81, "name": "group1977197923", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 23 | 33 | 71 | 72 | 73\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2\"", "from": "1977", "gid": "group1977197923", "height": "12.681", "label": "
TRANSITION | CORRELATION LENGTH ( 1977 , 1979 ) (((1977,1979),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
transition<\/TD> correlation length<\/TD> lattice gauge theories<\/TD> second order phase transition<\/TD><\/TR>\n
correlation functions<\/TD> expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | correlation functions | second order phase transition | lattice gauge theories | correlation length | transition\"", "nodeType": "group", "penwidth": "4", "pos": "24496,48456", "role": "\"1.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1979-10-09\"", "strTo": "\"1979-10-09\"", "support": "1", "to": "1979", "weight": "Just 1.0", "width": "12.681" }, { "_gvid": 82, "name": "group1977197924", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"26 | 54 | 62 | 63 | 64\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1977", "gid": "group1977197924", "height": "11.306", "label": "
REPLICA APPROACH | MEAN-FIELD MODEL ( 1977 , 1979 ) (((1977,1979),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica approach<\/TD> mean-field model<\/TD> order parameter<\/TD> spin glasses<\/TD><\/TR>\n
infinite number<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"infinite number | spin glasses | order parameter | mean-field model | replica approach\"", "nodeType": "group", "penwidth": "4", "pos": "12580,48456", "role": "\"1.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1979-10-09\"", "strTo": "\"1979-10-09\"", "support": "1", "to": "1979", "weight": "Just 1.0", "width": "11.306" }, { "_gvid": 83, "name": "group1977197925", "bId": "1", "branchId": "0 33 1 1 1 1 1", "fontname": "Arial", "foundation": "\"37 | 44 | 47\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1977", "gid": "group1977197925", "height": "7.8611", "label": "
HIGGS BOSON MASS | FERMIONS ( 1977 , 1979 ) (((1977,1979),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
higgs boson mass<\/TD> fermions<\/TD> energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | fermions | higgs boson mass\"", "nodeType": "group", "penwidth": "4", "pos": "3692.5,48456", "role": "\"3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1979-10-09\"", "strTo": "\"1979-10-09\"", "support": "1", "to": "1979", "weight": "Just 1.0", "width": "7.8611" }, { "_gvid": 84, "name": "group1977197926", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 55 | 56 | 57 | 58 | 59 | 60\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "1977", "gid": "group1977197926", "height": "12.25", "label": "
ENTROPY | ZERO TEMPERATURE ( 1977 , 1979 ) (((1977,1979),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
entropy<\/TD> zero temperature<\/TD> computer simulations<\/TD> specific heat<\/TD><\/TR>\n
internal energy<\/TD> sherrington-kirkpatrick model<\/TD> spin glasses<\/TD> mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | sherrington-kirkpatrick model | internal energy | specific heat | computer simulations | zero temperature | entropy\"", "nodeType": "group", "penwidth": "4", "pos": "14112,48456", "role": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1979-10-09\"", "strTo": "\"1979-10-09\"", "support": "1", "to": "1979", "weight": "Just 1.0", "width": "12.25" }, { "_gvid": 85, "name": "period19781980", "fontsize": "50", "from": "1978", "height": "0.875", "label": "1978 1980", "nodeType": "period", "pos": "33302,47446", "shape": "box", "strFrom": "\"1980-10-09\"", "strTo": "\"1980-10-09\"", "to": "1980", "width": "3.9444" }, { "_gvid": 86, "name": "group1978198020", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"5 | 54 | 55 | 64 | 81 | 83 | 84\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1978", "gid": "group1978198020", "height": "13.306", "label": "
MONTE CARLO SIMULATIONS | SPIN GLASS THEORY ( 1978 , 1980 ) (((1978,1980),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
monte carlo simulations<\/TD> spin glass theory<\/TD> spin glasses<\/TD> excellent agreement<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> replica approach<\/TD> theoretical predictions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"theoretical predictions | spin glasses | sherrington-kirkpatrick model | replica approach | excellent agreement | spin glass theory | monte carlo simulations\"", "nodeType": "group", "penwidth": "4", "pos": "13524,47446", "role": "\"0.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1980-10-09\"", "strTo": "\"1980-10-09\"", "support": "1", "to": "1980", "weight": "Just 1.0", "width": "13.306" }, { "_gvid": 87, "name": "group1978198024", "bId": "0", "branchId": "0 14 1 1", "fontname": "Arial", "foundation": "\"16 | 29 | 30 | 80\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1978", "gid": "group1978198024", "height": "11.486", "label": "
CONTINUUM LIMIT | COUPLING CONSTANTS ( 1978 , 1980 ) (((1978,1980),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
continuum limit<\/TD> coupling constants<\/TD> renormalization<\/TD> field theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization | coupling constants | field theories | continuum limit\"", "nodeType": "group", "penwidth": "4", "pos": "3109.5,47446", "role": "\"3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1980-10-09\"", "strTo": "\"1980-10-09\"", "support": "1", "to": "1980", "weight": "Just 1.0", "width": "11.486" }, { "_gvid": 88, "name": "group1978198025", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 58 | 62 | 75 | 76\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1978", "gid": "group1978198025", "height": "12.194", "label": "
CRITICAL TEMPERATURE | REPLICA SYMMETRY ( 1978 , 1980 ) (((1978,1980),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical temperature<\/TD> replica symmetry<\/TD> spin glasses<\/TD> computer simulations<\/TD><\/TR>\n
order parameter<\/TD> mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | computer simulations | order parameter | replica symmetry | critical temperature\"", "nodeType": "group", "penwidth": "4", "pos": "15696,47446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1980-10-09\"", "strTo": "\"1980-10-09\"", "support": "1", "to": "1980", "weight": "Just 1.0", "width": "12.194" }, { "_gvid": 89, "name": "group1978198026", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 57 | 87 | 88\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1978", "gid": "group1978198026", "height": "10.389", "label": "
SK MODEL | SPIN-GLASS PHASE ( 1978 , 1980 ) (((1978,1980),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sk model<\/TD> spin-glass phase<\/TD> specific heat<\/TD> mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | specific heat | spin-glass phase | sk model\"", "nodeType": "group", "penwidth": "4", "pos": "12598,47446", "role": "\"3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1980-10-09\"", "strTo": "\"1980-10-09\"", "support": "1", "to": "1980", "weight": "Just 1.0", "width": "10.389" }, { "_gvid": 90, "name": "group1978198027", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 55 | 58 | 62 | 69 | 75 | 76 | 81\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1978", "gid": "group1978198027", "height": "13.375", "label": "
SPIN GLASSES | CRITICAL TEMPERATURE ( 1978 , 1980 ) (((1978,1980),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> critical temperature<\/TD> replica symmetry<\/TD> computer simulations<\/TD><\/TR>\n
order parameter<\/TD> excellent agreement<\/TD> sherrington-kirkpatrick model<\/TD> external magnetic field<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | sherrington-kirkpatrick model | computer simulations | order parameter | external magnetic field | replica symmetry | critical temperature | excellent agreement\"", "nodeType": "group", "penwidth": "4", "pos": "14702,47446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1980-10-09\"", "strTo": "\"1980-10-09\"", "support": "1", "to": "1980", "weight": "Just 1.0", "width": "13.375" }, { "_gvid": 91, "name": "period19791981", "fontsize": "50", "from": "1979", "height": "0.875", "label": "1979 1981", "nodeType": "period", "pos": "33302,46334", "shape": "box", "strFrom": "\"1981-10-09\"", "strTo": "\"1981-10-09\"", "to": "1981", "width": "3.9444" }, { "_gvid": 92, "name": "group1979198121", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 33 | 37 | 67 | 71 | 73 | 84 | 91\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "1979", "gid": "group1979198121", "height": "15.486", "label": "
FIRST-ORDER TRANSITIONS | SECOND ORDER PHASE TRANSITION ( 1979 , 1981 ) (((1979,1981),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
first-order transitions<\/TD> second order phase transition<\/TD> transition<\/TD> lattice gauge theories<\/TD><\/TR>\n
critical points<\/TD> energy<\/TD> phase transition<\/TD> monte carlo simulations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | second order phase transition | energy | critical points | lattice gauge theories | transition | monte carlo simulations | first-order transitions\"", "nodeType": "group", "penwidth": "4", "pos": "23880,46334", "role": "\"3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1981-10-09\"", "strTo": "\"1981-10-09\"", "support": "1", "to": "1981", "weight": "Just 1.0", "width": "15.486" }, { "_gvid": 93, "name": "group1979198125", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 58 | 94 | 95 | 96\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1979", "gid": "group1979198125", "height": "11.972", "label": "
EQUILIBRIUM | LANGEVIN EQUATION ( 1979 , 1981 ) (((1979,1981),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
equilibrium<\/TD> langevin equation<\/TD> equilibrium properties<\/TD> computer simulations<\/TD><\/TR>\n
correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | computer simulations | equilibrium properties | langevin equation | equilibrium\"", "nodeType": "group", "penwidth": "4", "pos": "25088,46334", "role": "\"3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1981-10-09\"", "strTo": "\"1981-10-09\"", "support": "1", "to": "1981", "weight": "Just 1.0", "width": "11.972" }, { "_gvid": 94, "name": "group1979198128", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 39 | 53 | 54 | 55 | 60 | 70 | 81 | 87\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "1979", "gid": "group1979198128", "height": "13.292", "label": "
ENTROPY | SHERRINGTON-KIRKPATRICK MODEL ( 1979 , 1981 ) (((1979,1981),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
entropy<\/TD> sherrington-kirkpatrick model<\/TD> spin glasses<\/TD> spin-glass phase<\/TD><\/TR>\n
excellent agreement<\/TD> mean field theory<\/TD> magnetic field<\/TD> ground-state energy<\/TD><\/TR>\n
energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | ground-state energy | mean field theory | spin glasses | sherrington-kirkpatrick model | entropy | magnetic field | excellent agreement | spin-glass phase\"", "nodeType": "group", "penwidth": "4", "pos": "14112,46334", "role": "\"3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1981-10-09\"", "strTo": "\"1981-10-09\"", "support": "1", "to": "1981", "weight": "Just 1.0", "width": "13.292" }, { "_gvid": 95, "name": "group19791981210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"41 | 58 | 98 | 99\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1979", "gid": "group19791981210", "height": "13.486", "label": "
HADRONIC MASS SPECTRUM | HADRON MASSES ( 1979 , 1981 ) (((1979,1981),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hadronic mass spectrum<\/TD> hadron masses<\/TD> computer simulations<\/TD> quantum chromodynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"quantum chromodynamics | computer simulations | hadron masses | hadronic mass spectrum\"", "nodeType": "group", "penwidth": "4", "pos": "26076,46334", "role": "\"0.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1981-10-09\"", "strTo": "\"1981-10-09\"", "support": "1", "to": "1981", "weight": "Just 1.0", "width": "13.486" }, { "_gvid": 96, "name": "period19801982", "fontsize": "50", "from": "1980", "height": "0.875", "label": "1980 1982", "nodeType": "period", "pos": "33302,45315", "shape": "box", "strFrom": "\"1982-10-09\"", "strTo": "\"1982-10-09\"", "to": "1982", "width": "3.9444" }, { "_gvid": 97, "name": "group1980198220", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"3 | 23 | 71\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1980", "gid": "group1980198220", "height": "10.833", "label": "
MASS SPECTRUM | CORRELATION FUNCTIONS ( 1980 , 1982 ) (((1980,1982),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
correlation functions<\/TD> mass spectrum<\/TD> lattice gauge theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mass spectrum | correlation functions | lattice gauge theories\"", "nodeType": "group", "penwidth": "4", "pos": "24588,45315", "role": "\"0.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1982-10-09\"", "strTo": "\"1982-10-09\"", "support": "1", "to": "1982", "weight": "Just 1.0", "width": "10.833" }, { "_gvid": 98, "name": "group1980198221", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"10 | 37 | 104 | 106\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1980", "gid": "group1980198221", "height": "10.097", "label": "
QUENCHED APPROXIMATION | LATTICE QCD ( 1980 , 1982 ) (((1980,1982),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quenched approximation<\/TD> lattice qcd<\/TD> energy<\/TD> external field<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"external field | energy | lattice qcd | quenched approximation\"", "nodeType": "group", "penwidth": "4", "pos": "23058,45315", "role": "\"0.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1982-10-09\"", "strTo": "\"1982-10-09\"", "support": "1", "to": "1982", "weight": "Just 1.0", "width": "10.097" }, { "_gvid": 99, "name": "group1980198224", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 96 | 111\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1980", "gid": "group1980198224", "height": "8.7917", "label": "
NONLINEAR OSCILLATORS | EQUILIBRIUM ( 1980 , 1982 ) (((1980,1982),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
nonlinear oscillators<\/TD> equilibrium<\/TD> energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | equilibrium | nonlinear oscillators\"", "nodeType": "group", "penwidth": "4", "pos": "23810,45315", "role": "\"3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1982-10-09\"", "strTo": "\"1982-10-09\"", "support": "1", "to": "1982", "weight": "Just 1.0", "width": "8.7917" }, { "_gvid": 100, "name": "group1980198225", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"46 | 84 | 104 | 106\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1980", "gid": "group1980198225", "height": "10.75", "label": "
QUENCHED APPROXIMATION | LATTICE QCD ( 1980 , 1982 ) (((1980,1982),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quenched approximation<\/TD> lattice qcd<\/TD> monte carlo simulations<\/TD> qcd<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"qcd | monte carlo simulations | lattice qcd | quenched approximation\"", "nodeType": "group", "penwidth": "4", "pos": "22234,45315", "role": "\"3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1982-10-09\"", "strTo": "\"1982-10-09\"", "support": "1", "to": "1982", "weight": "Just 1.0", "width": "10.75" }, { "_gvid": 101, "name": "group1980198228", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"84 | 104 | 105\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1980", "gid": "group1980198228", "height": "8.9167", "label": "
QUARK MASS | LATTICE QCD ( 1980 , 1982 ) (((1980,1982),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quark mass<\/TD> lattice qcd<\/TD> monte carlo simulations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"monte carlo simulations | lattice qcd | quark mass\"", "nodeType": "group", "penwidth": "4", "pos": "26196,45315", "role": "\"3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1982-10-09\"", "strTo": "\"1982-10-09\"", "support": "1", "to": "1982", "weight": "Just 1.0", "width": "8.9167" }, { "_gvid": 102, "name": "period19811983", "fontsize": "50", "from": "1981", "height": "0.875", "label": "1981 1983", "nodeType": "period", "pos": "33302,44414", "shape": "box", "strFrom": "\"1983-10-09\"", "strTo": "\"1983-10-09\"", "to": "1983", "width": "3.9444" }, { "_gvid": 103, "name": "group1981198320", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"3 | 46 | 100 | 104 | 106\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1981", "gid": "group1981198320", "height": "9.2361", "label": "
QUENCHED APPROXIMATION | QCD ( 1981 , 1983 ) (((1981,1983),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quenched approximation<\/TD> qcd<\/TD> lattice qcd<\/TD> mass spectrum<\/TD><\/TR>\n
fluctuations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mass spectrum | qcd | fluctuations | lattice qcd | quenched approximation\"", "nodeType": "group", "penwidth": "4", "pos": "22646,44414", "role": "\"3.0 | 3.0 | 0.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1983-10-09\"", "strTo": "\"1983-10-09\"", "support": "1", "to": "1983", "weight": "Just 1.0", "width": "9.2361" }, { "_gvid": 104, "name": "group1981198321", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 41 | 44 | 84 | 104 | 105\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1981", "gid": "group1981198321", "height": "9.9722", "label": "
QUARK MASS | LATTICE QCD ( 1981 , 1983 ) (((1981,1983),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quark mass<\/TD> lattice qcd<\/TD> quantum chromodynamics<\/TD> fermions<\/TD><\/TR>\n
monte carlo simulations<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | quantum chromodynamics | fermions | monte carlo simulations | lattice qcd | quark mass\"", "nodeType": "group", "penwidth": "4", "pos": "26636,44414", "role": "\"3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1983-10-09\"", "strTo": "\"1983-10-09\"", "support": "1", "to": "1983", "weight": "Just 1.0", "width": "9.9722" }, { "_gvid": 105, "name": "group1981198323", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 71 | 95 | 96 | 115\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1981", "gid": "group1981198323", "height": "11.556", "label": "
GLUEBALL MASSES | LANGEVIN EQUATION ( 1981 , 1983 ) (((1981,1983),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glueball masses<\/TD> equilibrium<\/TD> langevin equation<\/TD> correlation functions<\/TD><\/TR>\n
lattice gauge theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | lattice gauge theories | langevin equation | equilibrium | glueball masses\"", "nodeType": "group", "penwidth": "4", "pos": "24838,44414", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1983-10-09\"", "strTo": "\"1983-10-09\"", "support": "1", "to": "1983", "weight": "Just 1.0", "width": "11.556" }, { "_gvid": 106, "name": "group1981198324", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"29 | 41 | 44 | 98 | 104 | 105\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1981", "gid": "group1981198324", "height": "12.208", "label": "
QUARK MASS | QUANTUM CHROMODYNAMICS ( 1981 , 1983 ) (((1981,1983),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quark mass<\/TD> quantum chromodynamics<\/TD> lattice qcd<\/TD> hadron masses<\/TD><\/TR>\n
fermions<\/TD> coupling constants<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"coupling constants | quantum chromodynamics | fermions | hadron masses | lattice qcd | quark mass\"", "nodeType": "group", "penwidth": "4", "pos": "25766,44414", "role": "\"1.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1983-10-09\"", "strTo": "\"1983-10-09\"", "support": "1", "to": "1983", "weight": "Just 1.0", "width": "12.208" }, { "_gvid": 107, "name": "group1981198325", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 62 | 64 | 117\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1981", "gid": "group1981198325", "height": "10.264", "label": "
REPLICAS | REPLICA APPROACH ( 1981 , 1983 ) (((1981,1983),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replicas<\/TD> replica approach<\/TD> order parameter<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | order parameter | replica approach | replicas\"", "nodeType": "group", "penwidth": "4", "pos": "15644,44414", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1983-10-09\"", "strTo": "\"1983-10-09\"", "support": "1", "to": "1983", "weight": "Just 1.0", "width": "10.264" }, { "_gvid": 108, "name": "group1981198326", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 62 | 116\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0\"", "from": "1981", "gid": "group1981198326", "height": "10.5", "label": "
PROBABILITY DISTRIBUTION | ORDER PARAMETER ( 1981 , 1983 ) (((1981,1983),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
probability distribution<\/TD> order parameter<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | order parameter | probability distribution\"", "nodeType": "group", "penwidth": "4", "pos": "14780,44414", "role": "\"3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1983-10-09\"", "strTo": "\"1983-10-09\"", "support": "1", "to": "1983", "weight": "Just 1.0", "width": "10.5" }, { "_gvid": 109, "name": "period19821984", "fontsize": "50", "from": "1982", "height": "0.875", "label": "1982 1984", "nodeType": "period", "pos": "33302,43430", "shape": "box", "strFrom": "\"1984-10-09\"", "strTo": "\"1984-10-09\"", "to": "1984", "width": "3.9444" }, { "_gvid": 110, "name": "group1982198420", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 53 | 54 | 131 | 132\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 3.7037037037037056e-2\"", "from": "1982", "gid": "group1982198420", "height": "11.5", "label": "
SPIN-GLASS MODEL | SELF-AVERAGING ( 1982 , 1984 ) (((1982,1984),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass model<\/TD> self-averaging<\/TD> mean field theory<\/TD> correlation functions<\/TD><\/TR>\n
spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | mean field theory | spin glasses | self-averaging | spin-glass model\"", "nodeType": "group", "penwidth": "4", "pos": "11192,43430", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1984-10-09\"", "strTo": "\"1984-10-09\"", "support": "1", "to": "1984", "weight": "Just 1.0", "width": "11.5" }, { "_gvid": 111, "name": "group1982198421", "bId": "1", "branchId": "0 33 1 1 1 1 1", "fontname": "Arial", "foundation": "\"36 | 37 | 44 | 124\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1982", "gid": "group1982198421", "height": "9.3056", "label": "
QUANTUM SYSTEM | GROUND STATE ( 1982 , 1984 ) (((1982,1984),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quantum system<\/TD> energy<\/TD> ground state<\/TD> fermions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground state | energy | fermions | quantum system\"", "nodeType": "group", "penwidth": "4", "pos": "3692.5,43430", "role": "\"1.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1984-10-09\"", "strTo": "\"1984-10-09\"", "support": "1", "to": "1984", "weight": "Just 1.0", "width": "9.3056" }, { "_gvid": 112, "name": "group1982198423", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 61 | 62 | 87 | 116 | 126 | 127 | 133\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1982", "gid": "group1982198423", "height": "13.111", "label": "
TOPOLOGY | THERMODYNAMICAL LIMIT ( 1982 , 1984 ) (((1982,1984),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
topology<\/TD> thermodynamical limit<\/TD> replica symmetry breaking<\/TD> probability distribution<\/TD><\/TR>\n
order parameter<\/TD> spin glasses<\/TD> spin-glass phase<\/TD> probability<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | probability | order parameter | spin-glass phase | probability distribution | thermodynamical limit | topology | replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "14692,43430", "role": "\"3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1984-10-09\"", "strTo": "\"1984-10-09\"", "support": "2", "to": "1984", "weight": "Just 2.0", "width": "13.111" }, { "_gvid": 113, "name": "group1982198425", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 64 | 117 | 137\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1982", "gid": "group1982198425", "height": "10.458", "label": "
THERMODYNAMICS | REPLICA APPROACH ( 1982 , 1984 ) (((1982,1984),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
thermodynamics<\/TD> replica approach<\/TD> spin glasses<\/TD> replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica approach | replicas | thermodynamics\"", "nodeType": "group", "penwidth": "4", "pos": "15634,43430", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1984-10-09\"", "strTo": "\"1984-10-09\"", "support": "1", "to": "1984", "weight": "Just 1.0", "width": "10.458" }, { "_gvid": 114, "name": "group1982198426", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 59 | 62 | 63 | 87 | 100 | 128 | 129 | 130\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1982", "gid": "group1982198426", "height": "12.139", "label": "
ULTRAMETRICITY | PURE STATES ( 1982 , 1984 ) (((1982,1984),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ultrametricity<\/TD> pure states<\/TD> overlap distributions<\/TD> mean-field model<\/TD><\/TR>\n
zero temperature<\/TD> sherrington-kirkpatrick model<\/TD> order parameter<\/TD> spin-glass phase<\/TD><\/TR>\n
fluctuations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | zero temperature | order parameter | mean-field model | spin-glass phase | fluctuations | overlap distributions | pure states | ultrametricity\"", "nodeType": "group", "penwidth": "4", "pos": "12116,43430", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1984-10-09\"", "strTo": "\"1984-10-09\"", "support": "1", "to": "1984", "weight": "Just 1.0", "width": "12.139" }, { "_gvid": 115, "name": "period19831985", "fontsize": "50", "from": "1983", "height": "0.875", "label": "1983 1985", "nodeType": "period", "pos": "33302,42484", "shape": "box", "strFrom": "\"1985-10-09\"", "strTo": "\"1985-10-09\"", "to": "1985", "width": "3.9444" }, { "_gvid": 116, "name": "group1983198521", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 75 | 117 | 139 | 140\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1983", "gid": "group1983198521", "height": "10.694", "label": "
MATCHING PROBLEM | BIPARTITIONS ( 1983 , 1985 ) (((1983,1985),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
matching problem<\/TD> bipartitions<\/TD> replica approach<\/TD> replica symmetry<\/TD><\/TR>\n
replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | replica symmetry | replicas | bipartitions | matching problem\"", "nodeType": "group", "penwidth": "4", "pos": "15524,42484", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1985-10-09\"", "strTo": "\"1985-10-09\"", "support": "1", "to": "1985", "weight": "Just 1.0", "width": "10.694" }, { "_gvid": 117, "name": "group1983198522", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"71 | 115 | 141 | 142\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1983", "gid": "group1983198522", "height": "11.181", "label": "
LATTICE SIZE | FINITE-SIZE EFFECT ( 1983 , 1985 ) (((1983,1985),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lattice size<\/TD> finite-size effect<\/TD> glueball masses<\/TD> lattice gauge theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"lattice gauge theories | glueball masses | finite-size effect | lattice size\"", "nodeType": "group", "penwidth": "4", "pos": "26040,42484", "role": "\"3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1985-10-09\"", "strTo": "\"1985-10-09\"", "support": "1", "to": "1985", "weight": "Just 1.0", "width": "11.181" }, { "_gvid": 118, "name": "period19841986", "fontsize": "50", "from": "1984", "height": "0.875", "label": "1984 1986", "nodeType": "period", "pos": "33302,41528", "shape": "box", "strFrom": "\"1986-10-09\"", "strTo": "\"1986-10-09\"", "to": "1986", "width": "3.9444" }, { "_gvid": 119, "name": "group1984198623", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 83 | 133 | 143\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1984", "gid": "group1984198623", "height": "11.403", "label": "
PHYSICAL MEANING | SPIN GLASS THEORY ( 1984 , 1986 ) (((1984,1986),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
physical meaning<\/TD> spin glass theory<\/TD> spin glasses<\/TD> mean field theory<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | spin glass theory | replica symmetry breaking | physical meaning\"", "nodeType": "group", "penwidth": "4", "pos": "14190,41528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1986-10-09\"", "strTo": "\"1986-10-09\"", "support": "1", "to": "1986", "weight": "Just 1.0", "width": "11.403" }, { "_gvid": 120, "name": "group1984198624", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 88 | 117 | 133\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1984", "gid": "group1984198624", "height": "13.375", "label": "
SK MODEL | SHERRINGTON-KIRKPATRICK MODEL ( 1984 , 1986 ) (((1984,1986),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sk model<\/TD> sherrington-kirkpatrick model<\/TD> replica symmetry breaking<\/TD> replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | sk model | replicas | replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "16116,41528", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1986-10-09\"", "strTo": "\"1986-10-09\"", "support": "1", "to": "1986", "weight": "Just 1.0", "width": "13.375" }, { "_gvid": 121, "name": "group1984198625", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 64 | 140\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1984", "gid": "group1984198625", "height": "10.319", "label": "
MATCHING PROBLEM | REPLICA APPROACH ( 1984 , 1986 ) (((1984,1986),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
matching problem<\/TD> replica approach<\/TD> mean-field model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | replica approach | matching problem\"", "nodeType": "group", "penwidth": "4", "pos": "15044,41528", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1986-10-09\"", "strTo": "\"1986-10-09\"", "support": "2", "to": "1986", "weight": "Just 2.0", "width": "10.319" }, { "_gvid": 122, "name": "period19851987", "fontsize": "50", "from": "1985", "height": "0.875", "label": "1985 1987", "nodeType": "period", "pos": "33302,40550", "shape": "box", "strFrom": "\"1987-10-09\"", "strTo": "\"1987-10-09\"", "to": "1987", "width": "3.9444" }, { "_gvid": 123, "name": "group1985198720", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 89 | 104 | 115 | 141\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1985", "gid": "group1985198720", "height": "10.597", "label": "
GLUEBALL MASSES | FINITE-SIZE EFFECT ( 1985 , 1987 ) (((1985,1987),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glueball masses<\/TD> finite-size effect<\/TD> string tension<\/TD> lattice qcd<\/TD><\/TR>\n
scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | string tension | lattice qcd | glueball masses | finite-size effect\"", "nodeType": "group", "penwidth": "4", "pos": "26312,40550", "role": "\"3.0 | 1.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1987-10-09\"", "strTo": "\"1987-10-09\"", "support": "1", "to": "1987", "weight": "Just 1.0", "width": "10.597" }, { "_gvid": 124, "name": "group1985198722", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 89 | 104 | 115\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1985", "gid": "group1985198722", "height": "10.972", "label": "
STRING TENSION | GLUEBALL MASSES ( 1985 , 1987 ) (((1985,1987),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
string tension<\/TD> glueball masses<\/TD> lattice qcd<\/TD> correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | string tension | lattice qcd | glueball masses\"", "nodeType": "group", "penwidth": "4", "pos": "24880,40550", "role": "\"3.0 | 1.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1987-10-09\"", "strTo": "\"1987-10-09\"", "support": "1", "to": "1987", "weight": "Just 1.0", "width": "10.972" }, { "_gvid": 125, "name": "group1985198723", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"39 | 53 | 54 | 75 | 83 | 139 | 151 | 152 | 153 | 154 | 155\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1985", "gid": "group1985198723", "height": "11.792", "label": "
FIXED CONNECTIVITY | RANDOM GRAPH ( 1985 , 1987 ) (((1985,1987),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fixed connectivity<\/TD> random graph<\/TD> random lattices<\/TD> ferromagnets<\/TD><\/TR>\n
finite connectivity<\/TD> bipartitions<\/TD> spin glasses<\/TD> spin glass theory<\/TD><\/TR>\n
replica symmetry<\/TD> mean field theory<\/TD> ground-state energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground-state energy | mean field theory | spin glasses | replica symmetry | spin glass theory | bipartitions | finite connectivity | ferromagnets | random lattices | random graph | fixed connectivity\"", "nodeType": "group", "penwidth": "4", "pos": "15306,40550", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1987-10-09\"", "strTo": "\"1987-10-09\"", "support": "1", "to": "1987", "weight": "Just 1.0", "width": "11.792" }, { "_gvid": 126, "name": "group1985198724", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 83 | 133 | 143 | 157\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1985", "gid": "group1985198724", "height": "11.111", "label": "
OPEN PROBLEMS | PHYSICAL MEANING ( 1985 , 1987 ) (((1985,1987),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
open problems<\/TD> physical meaning<\/TD> spin glass theory<\/TD> spin glasses<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | spin glass theory | replica symmetry breaking | physical meaning | open problems\"", "nodeType": "group", "penwidth": "4", "pos": "14300,40550", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1987-10-09\"", "strTo": "\"1987-10-09\"", "support": "1", "to": "1987", "weight": "Just 1.0", "width": "11.111" }, { "_gvid": 127, "name": "period19861988", "fontsize": "50", "from": "1986", "height": "0.875", "label": "1986 1988", "nodeType": "period", "pos": "33302,39576", "shape": "box", "strFrom": "\"1988-10-09\"", "strTo": "\"1988-10-09\"", "to": "1988", "width": "3.9444" }, { "_gvid": 128, "name": "group1986198820", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 41 | 89 | 104 | 108 | 115\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1986", "gid": "group1986198820", "height": "10.5", "label": "
LATTICE SPACING | LATTICE QCD ( 1986 , 1988 ) (((1986,1988),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lattice spacing<\/TD> lattice qcd<\/TD> scaling<\/TD> string tension<\/TD><\/TR>\n
glueball masses<\/TD> quantum chromodynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | quantum chromodynamics | string tension | lattice qcd | lattice spacing | glueball masses\"", "nodeType": "group", "penwidth": "4", "pos": "25106,39576", "role": "\"3.0 | 2.0 | 2.0 | 3.0 | 1.0 | 2.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1988-10-09\"", "strTo": "\"1988-10-09\"", "support": "1", "to": "1988", "weight": "Just 1.0", "width": "10.5" }, { "_gvid": 129, "name": "group1986198821", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 33 | 46 | 67 | 72 | 89 | 142 | 162\"", "frequence": "\"0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1986", "gid": "group1986198821", "height": "13.264", "label": "
STRONG FIRST-ORDER TRANSITION | LATTICE SIZE ( 1986 , 1988 ) (((1986,1988),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
strong first-order transition<\/TD> lattice size<\/TD> correlation length<\/TD> critical points<\/TD><\/TR>\n
qcd<\/TD> second order phase transition<\/TD> phase transition<\/TD> string tension<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | second order phase transition | qcd | critical points | correlation length | string tension | lattice size | strong first-order transition\"", "nodeType": "group", "penwidth": "4", "pos": "26476,39576", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1988-10-09\"", "strTo": "\"1988-10-09\"", "support": "1", "to": "1988", "weight": "Just 1.0", "width": "13.264" }, { "_gvid": 130, "name": "group1986198823", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"29 | 37 | 54 | 63 | 88 | 158 | 159\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1986", "gid": "group1986198823", "height": "10.375", "label": "
LOCAL MINIMA | LIMIT CYCLES ( 1986 , 1988 ) (((1986,1988),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
local minima<\/TD> limit cycles<\/TD> energy<\/TD> coupling constants<\/TD><\/TR>\n
sk model<\/TD> mean-field model<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"coupling constants | energy | spin glasses | mean-field model | sk model | limit cycles | local minima\"", "nodeType": "group", "penwidth": "4", "pos": "18754,39576", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1988-10-09\"", "strTo": "\"1988-10-09\"", "support": "1", "to": "1988", "weight": "Just 1.0", "width": "10.375" }, { "_gvid": 131, "name": "group1986198824", "bId": "2", "branchId": "0 45 1 1 1", "fontname": "Arial", "foundation": "\"99 | 160 | 161\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1986", "gid": "group1986198824", "height": "10.958", "label": "
CHIRAL LIMIT | QUENCHED LATTICE QCD ( 1986 , 1988 ) (((1986,1988),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
chiral limit<\/TD> quenched lattice qcd<\/TD> hadronic mass spectrum<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"hadronic mass spectrum | quenched lattice qcd | chiral limit\"", "nodeType": "group", "penwidth": "4", "pos": "5926.5,39576", "role": "\"1.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1988-10-09\"", "strTo": "\"1988-10-09\"", "support": "1", "to": "1988", "weight": "Just 1.0", "width": "10.958" }, { "_gvid": 132, "name": "period19871989", "fontsize": "50", "from": "1987", "height": "0.875", "label": "1987 1989", "nodeType": "period", "pos": "33302,38549", "shape": "box", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "to": "1989", "width": "3.9444" }, { "_gvid": 133, "name": "group1987198920", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 11 | 46 | 73 | 101 | 104 | 142\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1987", "gid": "group1987198920", "height": "9.8333", "label": "
CRITICAL BEHAVIOR | PHASE TRANSITION ( 1987 , 1989 ) (((1987,1989),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical behavior<\/TD> phase transition<\/TD> transition<\/TD> qcd<\/TD><\/TR>\n
lattice size<\/TD> scaling<\/TD> lattice qcd<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | phase transition | qcd | transition | critical behavior | lattice qcd | lattice size\"", "nodeType": "group", "penwidth": "4", "pos": "24666,38549", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "support": "1", "to": "1989", "weight": "Just 1.0", "width": "9.8333" }, { "_gvid": 134, "name": "group1987198921", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 23 | 67 | 72 | 73 | 142\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0\"", "from": "1987", "gid": "group1987198921", "height": "11", "label": "
PHASE TRANSITION | CORRELATION LENGTH ( 1987 , 1989 ) (((1987,1989),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
phase transition<\/TD> correlation length<\/TD> lattice size<\/TD> transition<\/TD><\/TR>\n
critical points<\/TD> correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | correlation functions | critical points | correlation length | transition | lattice size\"", "nodeType": "group", "penwidth": "4", "pos": "27378,38549", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "support": "1", "to": "1989", "weight": "Just 1.0", "width": "11" }, { "_gvid": 135, "name": "group1987198922", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 33 | 67 | 71 | 72 | 162 | 167\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "1987", "gid": "group1987198922", "height": "13.25", "label": "
SPATIAL DIMENSIONS | PHASE TRANSITION ( 1987 , 1989 ) (((1987,1989),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spatial dimensions<\/TD> phase transition<\/TD> strong first-order transition<\/TD> critical points<\/TD><\/TR>\n
correlation length<\/TD> second order phase transition<\/TD> lattice gauge theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | second order phase transition | critical points | lattice gauge theories | correlation length | strong first-order transition | spatial dimensions\"", "nodeType": "group", "penwidth": "4", "pos": "28322,38549", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "support": "1", "to": "1989", "weight": "Just 1.0", "width": "13.25" }, { "_gvid": 136, "name": "group1987198923", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 46 | 72 | 73 | 82 | 142 | 168\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1987", "gid": "group1987198923", "height": "12.181", "label": "
PHASE TRANSITION | CORRELATION LENGTH ( 1987 , 1989 ) (((1987,1989),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
phase transition<\/TD> correlation length<\/TD> spin models<\/TD> deconfinement transition<\/TD><\/TR>\n
transition<\/TD> lattice size<\/TD> qcd<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | qcd | correlation length | transition | spin models | lattice size | deconfinement transition\"", "nodeType": "group", "penwidth": "4", "pos": "25530,38549", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "support": "1", "to": "1989", "weight": "Just 1.0", "width": "12.181" }, { "_gvid": 137, "name": "group1987198924", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 72 | 142 | 162 | 168\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1987", "gid": "group1987198924", "height": "12.056", "label": "
PHASE TRANSITION | CORRELATION LENGTH ( 1987 , 1989 ) (((1987,1989),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
phase transition<\/TD> correlation length<\/TD> deconfinement transition<\/TD> lattice size<\/TD><\/TR>\n
strong first-order transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | correlation length | lattice size | strong first-order transition | deconfinement transition\"", "nodeType": "group", "penwidth": "4", "pos": "26476,38549", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "support": "1", "to": "1989", "weight": "Just 1.0", "width": "12.056" }, { "_gvid": 138, "name": "group1987198925", "bId": "2", "branchId": "0 45 1 1 1", "fontname": "Arial", "foundation": "\"46 | 99 | 148 | 160\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1987", "gid": "group1987198925", "height": "12.278", "label": "
HADRONIC MASS SPECTRUM | QUENCHED LATTICE QCD ( 1987 , 1989 ) (((1987,1989),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quenched lattice qcd<\/TD> hadronic mass spectrum<\/TD> ape computer<\/TD> qcd<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"qcd | hadronic mass spectrum | ape computer | quenched lattice qcd\"", "nodeType": "group", "penwidth": "4", "pos": "5650.5,38549", "role": "\"1.0 | 2.0 | 0.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "support": "1", "to": "1989", "weight": "Just 1.0", "width": "12.278" }, { "_gvid": 139, "name": "group1987198926", "bId": "3", "branchId": "0 46 1 1 1 1 1 1", "fontname": "Arial", "foundation": "\"54 | 145 | 163\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0\"", "from": "1987", "gid": "group1987198926", "height": "9.1528", "label": "
NEURAL NETWORK | SPIN GLASSES ( 1987 , 1989 ) (((1987,1989),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
neural network<\/TD> spin glasses<\/TD> idiotypic network<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | neural network | idiotypic network\"", "nodeType": "group", "penwidth": "4", "pos": "7929.5,38549", "role": "\"1.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1989-10-09\"", "strTo": "\"1989-10-09\"", "support": "1", "to": "1989", "weight": "Just 1.0", "width": "9.1528" }, { "_gvid": 140, "name": "period19881990", "fontsize": "50", "from": "1988", "height": "0.875", "label": "1988 1990", "nodeType": "period", "pos": "33302,37502", "shape": "box", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "to": "1990", "width": "3.9444" }, { "_gvid": 141, "name": "group1988199021", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 44 | 46 | 108 | 125\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1988", "gid": "group1988199021", "height": "9.6944", "label": "
SCALING | LATTICE SPACING ( 1988 , 1990 ) (((1988,1990),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling<\/TD> lattice spacing<\/TD> fermions<\/TD> staggered fermions<\/TD><\/TR>\n
qcd<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | fermions | qcd | lattice spacing | staggered fermions\"", "nodeType": "group", "penwidth": "4", "pos": "24208,37502", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "9.6944" }, { "_gvid": 142, "name": "group1988199022", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 64 | 102 | 134 | 169\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1988", "gid": "group1988199022", "height": "9.0972", "label": "
DISORDER | POLYMER ( 1988 , 1990 ) (((1988,1990),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
disorder<\/TD> polymer<\/TD> replica approach<\/TD> critical exponents<\/TD><\/TR>\n
random media<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | replica approach | polymer | disorder | random media\"", "nodeType": "group", "penwidth": "4", "pos": "12804,37502", "role": "\"1.0 | 3.0 | 1.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "9.0972" }, { "_gvid": 143, "name": "group1988199023", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 54 | 55 | 87 | 117\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1988", "gid": "group1988199023", "height": "11.278", "label": "
REPLICAS | SPIN-GLASS PHASE ( 1988 , 1990 ) (((1988,1990),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replicas<\/TD> spin-glass phase<\/TD> sherrington-kirkpatrick model<\/TD> spin glasses<\/TD><\/TR>\n
correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | spin glasses | sherrington-kirkpatrick model | spin-glass phase | replicas\"", "nodeType": "group", "penwidth": "4", "pos": "15936,37502", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "11.278" }, { "_gvid": 144, "name": "group1988199024", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 56 | 58 | 70 | 116 | 130 | 136\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1988", "gid": "group1988199024", "height": "12.444", "label": "
ULTRAMETRICITY | PROBABILITY DISTRIBUTION ( 1988 , 1990 ) (((1988,1990),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ultrametricity<\/TD> probability distribution<\/TD> spin glasses<\/TD> mean field theory<\/TD><\/TR>\n
magnetic field<\/TD> computer simulations<\/TD> internal energy<\/TD> ising spin-glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | internal energy | computer simulations | magnetic field | probability distribution | ultrametricity | ising spin-glasses\"", "nodeType": "group", "penwidth": "4", "pos": "17920,37502", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "12.444" }, { "_gvid": 145, "name": "group1988199025", "bId": "3", "branchId": "0 46 1 1 1 1 1 1", "fontname": "Arial", "foundation": "\"63 | 145 | 174\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1988", "gid": "group1988199025", "height": "10.889", "label": "
INFORMA UK LTD ALL RIGHTS | MEAN-FIELD MODEL ( 1988 , 1990 ) (((1988,1990),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
informa uk ltd all rights<\/TD> neural network<\/TD> mean-field model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | neural network | informa uk ltd all rights\"", "nodeType": "group", "penwidth": "4", "pos": "7050.5,37502", "role": "\"1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "10.889" }, { "_gvid": 146, "name": "group1988199026", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"65 | 75 | 97 | 102 | 133 | 169 | 170\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1988", "gid": "group1988199026", "height": "13.819", "label": "
VARIATIONAL APPROACH | REPLICA SYMMETRY BREAKING ( 1988 , 1990 ) (((1988,1990),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
variational approach<\/TD> replica symmetry breaking<\/TD> ising model<\/TD> replica symmetry<\/TD><\/TR>\n
random magnetic fields<\/TD> polymer<\/TD> random media<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"random magnetic fields | replica symmetry | ising model | polymer | replica symmetry breaking | random media | variational approach\"", "nodeType": "group", "penwidth": "4", "pos": "13700,37502", "role": "\"1.0 | 3.0 | 1.0 | 1.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "13.819" }, { "_gvid": 147, "name": "group1988199028", "bId": "2", "branchId": "0 45 1 1 1", "fontname": "Arial", "foundation": "\"81 | 100 | 142 | 160 | 161\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1988", "gid": "group1988199028", "height": "10.694", "label": "
CHIRAL LIMIT | FLUCTUATIONS ( 1988 , 1990 ) (((1988,1990),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
chiral limit<\/TD> quenched lattice qcd<\/TD> fluctuations<\/TD> excellent agreement<\/TD><\/TR>\n
lattice size<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"excellent agreement | fluctuations | lattice size | quenched lattice qcd | chiral limit\"", "nodeType": "group", "penwidth": "4", "pos": "6201.5,37502", "role": "\"1.0 | 1.0 | 1.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "10.694" }, { "_gvid": 148, "name": "group1988199029", "bId": "3", "branchId": "0 46 1 1 1 1 1 1", "fontname": "Arial", "foundation": "\"132 | 145 | 163 | 173\"", "frequence": "\"3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1988", "gid": "group1988199029", "height": "11.528", "label": "
MEMORY CAPACITY | IDIOTYPIC NETWORK ( 1988 , 1990 ) (((1988,1990),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
memory capacity<\/TD> idiotypic network<\/TD> neural network<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass model | neural network | idiotypic network | memory capacity\"", "nodeType": "group", "penwidth": "4", "pos": "7929.5,37502", "role": "\"1.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1990-10-09\"", "strTo": "\"1990-10-09\"", "support": "1", "to": "1990", "weight": "Just 1.0", "width": "11.528" }, { "_gvid": 149, "name": "period19891991", "fontsize": "50", "from": "1989", "height": "0.875", "label": "1989 1991", "nodeType": "period", "pos": "33302,36434", "shape": "box", "strFrom": "\"1991-10-09\"", "strTo": "\"1991-10-09\"", "to": "1991", "width": "3.9444" }, { "_gvid": 150, "name": "group1989199120", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 73 | 81 | 182\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "1989", "gid": "group1989199120", "height": "12.903", "label": "
DYNAMICAL PHASE TRANSITION | EXCELLENT AGREEMENT ( 1989 , 1991 ) (((1989,1991),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical phase transition<\/TD> excellent agreement<\/TD> transition<\/TD> critical exponents<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | transition | excellent agreement | dynamical phase transition\"", "nodeType": "group", "penwidth": "4", "pos": "23400,36434", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1991-10-09\"", "strTo": "\"1991-10-09\"", "support": "1", "to": "1991", "weight": "Just 1.0", "width": "12.903" }, { "_gvid": 151, "name": "group1989199121", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 102 | 170 | 175 | 176\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1989", "gid": "group1989199121", "height": "9.7917", "label": "
SELF-REPULSION | POLYMER ( 1989 , 1991 ) (((1989,1991),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
self-repulsion<\/TD> polymer<\/TD> variational approach<\/TD> self-interacting<\/TD><\/TR>\n
critical exponents<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | polymer | variational approach | self-repulsion | self-interacting\"", "nodeType": "group", "penwidth": "4", "pos": "12804,36434", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1991-10-09\"", "strTo": "\"1991-10-09\"", "support": "1", "to": "1991", "weight": "Just 1.0", "width": "9.7917" }, { "_gvid": 152, "name": "group1989199122", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"31 | 58 | 73 | 101 | 180 | 181\"", "frequence": "\"0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1989", "gid": "group1989199122", "height": "13.847", "label": "
GLASSY SYSTEMS | STRETCHED EXPONENTIAL RELAXATION ( 1989 , 1991 ) (((1989,1991),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glassy systems<\/TD> stretched exponential relaxation<\/TD> critical behavior<\/TD> transition<\/TD><\/TR>\n
computer simulations<\/TD> divergence<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"divergence | computer simulations | transition | critical behavior | stretched exponential relaxation | glassy systems\"", "nodeType": "group", "penwidth": "4", "pos": "24434,36434", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1991-10-09\"", "strTo": "\"1991-10-09\"", "support": "1", "to": "1991", "weight": "Just 1.0", "width": "13.847" }, { "_gvid": 153, "name": "group1989199124", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 84 | 87 | 133\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1989", "gid": "group1989199124", "height": "12.111", "label": "
SPIN-GLASS PHASE | SPIN GLASSES ( 1989 , 1991 ) (((1989,1991),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass phase<\/TD> spin glasses<\/TD> replica symmetry breaking<\/TD> monte carlo simulations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | monte carlo simulations | spin-glass phase | replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "14564,36434", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1991-10-09\"", "strTo": "\"1991-10-09\"", "support": "1", "to": "1991", "weight": "Just 1.0", "width": "12.111" }, { "_gvid": 154, "name": "group1989199125", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"75 | 116 | 117\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1989", "gid": "group1989199125", "height": "10.375", "label": "
REPLICAS | PROBABILITY DISTRIBUTION ( 1989 , 1991 ) (((1989,1991),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replicas<\/TD> probability distribution<\/TD> replica symmetry<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica symmetry | probability distribution | replicas\"", "nodeType": "group", "penwidth": "4", "pos": "11920,36434", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1991-10-09\"", "strTo": "\"1991-10-09\"", "support": "1", "to": "1991", "weight": "Just 1.0", "width": "10.375" }, { "_gvid": 155, "name": "group1989199126", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"84 | 176 | 177 | 178 | 179\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1989", "gid": "group1989199126", "height": "12.264", "label": "
MONOMERS | THERMODYNAMIC BEHAVIOUR ( 1989 , 1991 ) (((1989,1991),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
monomers<\/TD> thermodynamic behaviour<\/TD> protein folding<\/TD> self-interacting<\/TD><\/TR>\n
monte carlo simulations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"monte carlo simulations | self-interacting | protein folding | thermodynamic behaviour | monomers\"", "nodeType": "group", "penwidth": "4", "pos": "19306,36434", "role": "\"3.0 | 2.0 | 2.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1991-10-09\"", "strTo": "\"1991-10-09\"", "support": "1", "to": "1991", "weight": "Just 1.0", "width": "12.264" }, { "_gvid": 156, "name": "period19901992", "fontsize": "50", "from": "1990", "height": "0.875", "label": "1990 1992", "nodeType": "period", "pos": "33302,35345", "shape": "box", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "to": "1992", "width": "3.9444" }, { "_gvid": 157, "name": "group1990199220", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"1 | 107 | 133 | 190\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group1990199220", "height": "13.389", "label": "
EQUILIBRIUM STATES | REPLICA SYMMETRY BREAKING ( 1990 , 1992 ) (((1990,1992),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
equilibrium states<\/TD> replica symmetry breaking<\/TD> free energy<\/TD> symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"symmetry breaking | free energy | replica symmetry breaking | equilibrium states\"", "nodeType": "group", "penwidth": "4", "pos": "13054,35345", "role": "\"3.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "13.389" }, { "_gvid": 158, "name": "group1990199221", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"3 | 4 | 104 | 148 | 161\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group1990199221", "height": "9.4028", "label": "
APE COMPUTER | LATTICE QCD ( 1990 , 1992 ) (((1990,1992),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ape computer<\/TD> lattice qcd<\/TD> mass spectrum<\/TD> chiral limit<\/TD><\/TR>\n
scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mass spectrum | scaling | lattice qcd | ape computer | chiral limit\"", "nodeType": "group", "penwidth": "4", "pos": "24834,35345", "role": "\"2.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "9.4028" }, { "_gvid": 159, "name": "group1990199222", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 73 | 100 | 169 | 192\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group1990199222", "height": "10.986", "label": "
SURFACE GROWTH | CRITICAL EXPONENTS ( 1990 , 1992 ) (((1990,1992),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
surface growth<\/TD> critical exponents<\/TD> transition<\/TD> random media<\/TD><\/TR>\n
fluctuations<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | transition | fluctuations | random media | surface growth\"", "nodeType": "group", "penwidth": "4", "pos": "23818,35345", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "10.986" }, { "_gvid": 160, "name": "group1990199223", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 37 | 191\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0\"", "from": "1990", "gid": "group1990199223", "height": "8.4028", "label": "
INTERMITTENCY CORRECTION | ENERGY ( 1990 , 1992 ) (((1990,1992),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
intermittency correction<\/TD> energy<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | energy | intermittency correction\"", "nodeType": "group", "penwidth": "4", "pos": "18332,35345", "role": "\"3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "8.4028" }, { "_gvid": 161, "name": "group1990199224", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"30 | 98 | 104 | 110 | 141 | 184\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group1990199224", "height": "10.222", "label": "
FINITE LATTICE | FINITE-SIZE EFFECT ( 1990 , 1992 ) (((1990,1992),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-size effect<\/TD> finite lattice<\/TD> hadron masses<\/TD> field theories<\/TD><\/TR>\n
lattice qcd<\/TD> power law<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"field theories | hadron masses | lattice qcd | finite lattice | finite-size effect | power law\"", "nodeType": "group", "penwidth": "4", "pos": "28908,35345", "role": "\"1.0 | 3.0 | 3.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "10.222" }, { "_gvid": 162, "name": "group1990199225", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 88 | 130 | 132\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 3.7037037037037056e-2\"", "from": "1990", "gid": "group1990199225", "height": "9.0417", "label": "
ULTRAMETRICITY | SK MODEL ( 1990 , 1992 ) (((1990,1992),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ultrametricity<\/TD> sk model<\/TD> energy<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | sk model | ultrametricity | spin-glass model\"", "nodeType": "group", "penwidth": "4", "pos": "19032,35345", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "9.0417" }, { "_gvid": 163, "name": "group1990199226", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 67 | 88 | 100 | 107 | 126 | 183\"", "frequence": "\"5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1990", "gid": "group1990199226", "height": "12.292", "label": "
MEAN-FIELD SOLUTION | THERMODYNAMICAL LIMIT ( 1990 , 1992 ) (((1990,1992),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mean-field solution<\/TD> thermodynamical limit<\/TD> critical points<\/TD> spin glasses<\/TD><\/TR>\n
sk model<\/TD> fluctuations<\/TD> free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | critical points | sk model | fluctuations | free energy | thermodynamical limit | mean-field solution\"", "nodeType": "group", "penwidth": "4", "pos": "16488,35345", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "12.292" }, { "_gvid": 164, "name": "group1990199227", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 62 | 107 | 132 | 137 | 189\"", "frequence": "\"0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "1990", "gid": "group1990199227", "height": "11.764", "label": "
FINITE-SIZE CORRECTIONS | THERMODYNAMICS ( 1990 , 1992 ) (((1990,1992),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-size corrections<\/TD> thermodynamics<\/TD> free energy<\/TD> order parameter<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | order parameter | free energy | spin-glass model | thermodynamics | finite-size corrections\"", "nodeType": "group", "penwidth": "4", "pos": "14032,35345", "role": "\"3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "11.764" }, { "_gvid": 165, "name": "group1990199228", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"61 | 102 | 107 | 116 | 117 | 133 | 169 | 170\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group1990199228", "height": "12.042", "label": "
POLYMER | VARIATIONAL APPROACH ( 1990 , 1992 ) (((1990,1992),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
polymer<\/TD> variational approach<\/TD> random media<\/TD> replica symmetry breaking<\/TD><\/TR>\n
probability distribution<\/TD> replicas<\/TD> free energy<\/TD> probability<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"probability | polymer | free energy | probability distribution | replicas | replica symmetry breaking | random media | variational approach\"", "nodeType": "group", "penwidth": "4", "pos": "11920,35345", "role": "\"3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "12.042" }, { "_gvid": 166, "name": "group1990199229", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 64 | 65 | 117 | 152\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group1990199229", "height": "12.722", "label": "
FERROMAGNETS | RANDOM MAGNETIC FIELDS ( 1990 , 1992 ) (((1990,1992),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ferromagnets<\/TD> random magnetic fields<\/TD> replica approach<\/TD> mean-field model<\/TD><\/TR>\n
replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | replica approach | random magnetic fields | replicas | ferromagnets\"", "nodeType": "group", "penwidth": "4", "pos": "21456,35345", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "12.722" }, { "_gvid": 167, "name": "group19901992210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"84 | 138 | 179\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group19901992210", "height": "11.417", "label": "
MONTE CARLO SIMULATIONS | STATISTICAL MECHANICS ( 1990 , 1992 ) (((1990,1992),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
monte carlo simulations<\/TD> monomers<\/TD> statistical mechanics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"monte carlo simulations | statistical mechanics | monomers\"", "nodeType": "group", "penwidth": "4", "pos": "19840,35345", "role": "\"3.0 | 1.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "11.417" }, { "_gvid": 168, "name": "group19901992211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"88 | 107 | 137 | 189\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group19901992211", "height": "11.222", "label": "
FINITE-SIZE CORRECTIONS | THERMODYNAMICS ( 1990 , 1992 ) (((1990,1992),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-size corrections<\/TD> thermodynamics<\/TD> free energy<\/TD> sk model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sk model | free energy | thermodynamics | finite-size corrections\"", "nodeType": "group", "penwidth": "4", "pos": "17408,35345", "role": "\"3.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "11.222" }, { "_gvid": 169, "name": "group19901992212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"96 | 185 | 186 | 187 | 188\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1990", "gid": "group19901992212", "height": "14.417", "label": "
RANDOM-FIELD ISING MODEL | FREE-ENERGY LANDSCAPE ( 1990 , 1992 ) (((1990,1992),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random-field ising model<\/TD> nonzero temperature<\/TD> free-energy landscape<\/TD> simulated tempering<\/TD><\/TR>\n
equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"equilibrium | simulated tempering | free-energy landscape | nonzero temperature | random-field ising model\"", "nodeType": "group", "penwidth": "4", "pos": "15308,35345", "role": "\"3.0 | 2.0 | 0.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1992-10-09\"", "strTo": "\"1992-10-09\"", "support": "1", "to": "1992", "weight": "Just 1.0", "width": "14.417" }, { "_gvid": 170, "name": "period19911993", "fontsize": "50", "from": "1991", "height": "0.875", "label": "1991 1993", "nodeType": "period", "pos": "33302,34252", "shape": "box", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "to": "1993", "width": "3.9444" }, { "_gvid": 171, "name": "group1991199321", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 37 | 87 | 116 | 130 | 136\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1991", "gid": "group1991199321", "height": "10.722", "label": "
ENERGY | ISING SPIN-GLASSES ( 1991 , 1993 ) (((1991,1993),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
energy<\/TD> ising spin-glasses<\/TD> spin-glass phase<\/TD> ultrametricity<\/TD><\/TR>\n
scaling<\/TD> probability distribution<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | energy | spin-glass phase | probability distribution | ultrametricity | ising spin-glasses\"", "nodeType": "group", "penwidth": "4", "pos": "18164,34252", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "10.722" }, { "_gvid": 172, "name": "group1991199322", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 54 | 69 | 136 | 150 | 201\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1991", "gid": "group1991199322", "height": "10.042", "label": "
4D | CRITICAL LINE ( 1991 , 1993 ) (((1991,1993),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
4d<\/TD> critical line<\/TD> external magnetic field<\/TD> critical exponents<\/TD><\/TR>\n
spin glasses<\/TD> ising spin-glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | spin glasses | external magnetic field | ising spin-glasses | critical line | 4d\"", "nodeType": "group", "penwidth": "4", "pos": "9606.5,34252", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "10.042" }, { "_gvid": 173, "name": "group1991199323", "bId": "3", "branchId": "0 46 1 1 1 1 1 1", "fontname": "Arial", "foundation": "\"10 | 145 | 146 | 174\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1991", "gid": "group1991199323", "height": "11.569", "label": "
SYNAPTIC STRENGTHS | EXTERNAL FIELD ( 1991 , 1993 ) (((1991,1993),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
synaptic strengths<\/TD> neural network<\/TD> external field<\/TD> informa uk ltd all rights<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"external field | neural network | synaptic strengths | informa uk ltd all rights\"", "nodeType": "group", "penwidth": "4", "pos": "7050.5,34252", "role": "\"1.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "11.569" }, { "_gvid": 174, "name": "group1991199324", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 102 | 169 | 193 | 194\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1991", "gid": "group1991199324", "height": "7.7639", "label": "
TOY MODEL | AGING ( 1991 , 1993 ) (((1991,1993),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
toy model<\/TD> aging<\/TD> random media<\/TD> polymer<\/TD><\/TR>\n
correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | polymer | random media | aging | toy model\"", "nodeType": "group", "penwidth": "4", "pos": "7818.5,34252", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "7.7639" }, { "_gvid": 175, "name": "group1991199326", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"46 | 98 | 110 | 141 | 184\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1991", "gid": "group1991199326", "height": "10.181", "label": "
FINITE LATTICE | HADRON MASSES ( 1991 , 1993 ) (((1991,1993),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite lattice<\/TD> hadron masses<\/TD> power law<\/TD> finite-size effect<\/TD><\/TR>\n
qcd<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"qcd | hadron masses | finite lattice | finite-size effect | power law\"", "nodeType": "group", "penwidth": "4", "pos": "28908,34252", "role": "\"3.0 | 2.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "10.181" }, { "_gvid": 176, "name": "group1991199327", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"51 | 54 | 80 | 112 | 127 | 197\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1991", "gid": "group1991199327", "height": "10.528", "label": "
BIFURCATION | UNIVERSAL ( 1991 , 1993 ) (((1991,1993),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
bifurcation<\/TD> topology<\/TD> universal<\/TD> continuum limit<\/TD><\/TR>\n
spin glasses<\/TD> plenum publishing corporation<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"plenum publishing corporation | spin glasses | continuum limit | universal | topology | bifurcation\"", "nodeType": "group", "penwidth": "4", "pos": "10420,34252", "role": "\"1.0 | 3.0 | 2.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "10.528" }, { "_gvid": 177, "name": "group1991199328", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 107 | 130 | 132 | 198 | 199 | 200\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1991", "gid": "group1991199328", "height": "11.472", "label": "
MEAN-FIELD SPIN GLASSES | REAL REPLICAS ( 1991 , 1993 ) (((1991,1993),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mean-field spin glasses<\/TD> real replicas<\/TD> free energy cost<\/TD> spin-glass model<\/TD><\/TR>\n
ultrametricity<\/TD> free energy<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | free energy | ultrametricity | spin-glass model | free energy cost | real replicas | mean-field spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "16484,34252", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "11.472" }, { "_gvid": 178, "name": "group1991199329", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 133 | 143 | 156\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1991", "gid": "group1991199329", "height": "12.639", "label": "
PHYSICAL MEANING | REPLICA SYMMETRY BREAKING ( 1991 , 1993 ) (((1991,1993),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
physical meaning<\/TD> replica symmetry breaking<\/TD> spin glasses<\/TD> complexity<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica symmetry breaking | physical meaning | complexity\"", "nodeType": "group", "penwidth": "4", "pos": "14094,34252", "role": "\"3.0 | 3.0 | 3.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "12.639" }, { "_gvid": 179, "name": "group19911993210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"56 | 73 | 87 | 88 | 130 | 132 | 189\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "1991", "gid": "group19911993210", "height": "11.347", "label": "
SPIN-GLASS MODEL | ULTRAMETRICITY ( 1991 , 1993 ) (((1991,1993),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass model<\/TD> ultrametricity<\/TD> sk model<\/TD> finite-size corrections<\/TD><\/TR>\n
spin-glass phase<\/TD> transition<\/TD> internal energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"internal energy | transition | spin-glass phase | sk model | ultrametricity | spin-glass model | finite-size corrections\"", "nodeType": "group", "penwidth": "4", "pos": "19032,34252", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "11.347" }, { "_gvid": 180, "name": "group19911993212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"87 | 117 | 133 | 136 | 195\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1991", "gid": "group19911993212", "height": "13.931", "label": "
FOUR-DIMENSIONAL SPIN GLASS | ISING SPIN-GLASSES ( 1991 , 1993 ) (((1991,1993),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
four-dimensional spin glass<\/TD> ising spin-glasses<\/TD> spin-glass phase<\/TD> replica symmetry breaking<\/TD><\/TR>\n
replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass phase | replicas | replica symmetry breaking | ising spin-glasses | four-dimensional spin glass\"", "nodeType": "group", "penwidth": "4", "pos": "8671.5,34252", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1993-10-09\"", "strTo": "\"1993-10-09\"", "support": "1", "to": "1993", "weight": "Just 1.0", "width": "13.931" }, { "_gvid": 181, "name": "period19921994", "fontsize": "50", "from": "1992", "height": "0.875", "label": "1992 1994", "nodeType": "period", "pos": "33302,33150", "shape": "box", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "to": "1994", "width": "3.9444" }, { "_gvid": 182, "name": "group1992199420", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 51 | 63 | 84 | 85 | 211 | 212\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1992", "gid": "group1992199420", "height": "13.819", "label": "
SHORT-RANGE INTERACTION | SELF-AVOIDING ( 1992 , 1994 ) (((1992,1994),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
self-repelling random walks<\/TD> short-range interaction<\/TD> self-avoiding<\/TD> monte carlo simulations<\/TD><\/TR>\n
scaling<\/TD> plenum publishing corporation<\/TD> mean-field model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | plenum publishing corporation | mean-field model | monte carlo simulations | self-avoiding | short-range interaction | self-repelling random walks\"", "nodeType": "group", "penwidth": "4", "pos": "29592,33150", "role": "\"3.0 | 2.0 | 3.0 | 3.0 | 1.0 | 0.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "13.819" }, { "_gvid": 183, "name": "group1992199421", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 77 | 84 | 190 | 218\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1992", "gid": "group1992199421", "height": "10.694", "label": "
EXTERNAL PERTURBATION | SCALING ( 1992 , 1994 ) (((1992,1994),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
external perturbation<\/TD> scaling<\/TD> disordered systems<\/TD> equilibrium states<\/TD><\/TR>\n
monte carlo simulations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | disordered systems | monte carlo simulations | equilibrium states | external perturbation\"", "nodeType": "group", "penwidth": "4", "pos": "28636,33150", "role": "\"3.0 | 0.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "10.694" }, { "_gvid": 184, "name": "group1992199422", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"12 | 54 | 63 | 193 | 219 | 220\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1992", "gid": "group1992199422", "height": "12.153", "label": "
EQUILIBRIUM DYNAMICS | UNFRUSTRATED SYSTEMS ( 1992 , 1994 ) (((1992,1994),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
unfrustrated systems<\/TD> equilibrium dynamics<\/TD> aging<\/TD> mean-field model<\/TD><\/TR>\n
spin glasses<\/TD> asymptotic behaviour<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"asymptotic behaviour | spin glasses | mean-field model | aging | equilibrium dynamics | unfrustrated systems\"", "nodeType": "group", "penwidth": "4", "pos": "5063.5,33150", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 0.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "12.153" }, { "_gvid": 185, "name": "group1992199423", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"30 | 54 | 87 | 117 | 149 | 202 | 203 | 204\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1992", "gid": "group1992199423", "height": "12", "label": "
DISORDERED MODEL | QUENCHED DISORDER ( 1992 , 1994 ) (((1992,1994),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
disordered model<\/TD> complex landscape<\/TD> quenched disorder<\/TD> replicas<\/TD><\/TR>\n
field theories<\/TD> phase diagram<\/TD> spin-glass phase<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"field theories | spin glasses | spin-glass phase | replicas | phase diagram | quenched disorder | complex landscape | disordered model\"", "nodeType": "group", "penwidth": "4", "pos": "15936,33150", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "12" }, { "_gvid": 186, "name": "group1992199424", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"30 | 64 | 117 | 202 | 203\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1992", "gid": "group1992199424", "height": "11.181", "label": "
QUENCHED DISORDER | COMPLEX LANDSCAPE ( 1992 , 1994 ) (((1992,1994),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
complex landscape<\/TD> quenched disorder<\/TD> field theories<\/TD> replicas<\/TD><\/TR>\n
replica approach<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"field theories | replica approach | replicas | quenched disorder | complex landscape\"", "nodeType": "group", "penwidth": "4", "pos": "21456,33150", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "11.181" }, { "_gvid": 187, "name": "group1992199425", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"34 | 54 | 63 | 70 | 138 | 144 | 205 | 206 | 207 | 208 | 209\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1992", "gid": "group1992199425", "height": "14.681", "label": "
TRANSITION POINT | THERMODYNAMIC PROPERTIES ( 1992 , 1994 ) (((1992,1994),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
transition point<\/TD> thermodynamic properties<\/TD> oscillators<\/TD> josephson junctions<\/TD><\/TR>\n
d-dimensional array<\/TD> matrix elements<\/TD> magnetic field<\/TD> statistical mechanics<\/TD><\/TR>\n
mean-field model<\/TD> spin glasses<\/TD> high temperature expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"high temperature expansion | spin glasses | mean-field model | magnetic field | statistical mechanics | matrix elements | d-dimensional array | josephson junctions | oscillators | thermodynamic properties | transition point\"", "nodeType": "group", "penwidth": "4", "pos": "14420,33150", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "14.681" }, { "_gvid": 188, "name": "group1992199426", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 75 | 107 | 132 | 133 | 135\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "1992", "gid": "group1992199426", "height": "11.597", "label": "
LOWER CRITICAL DIMENSION | SPIN GLASSES ( 1992 , 1994 ) (((1992,1994),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lower critical dimension<\/TD> spin glasses<\/TD> free energy<\/TD> replica symmetry<\/TD><\/TR>\n
replica symmetry breaking<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica symmetry | free energy | spin-glass model | replica symmetry breaking | lower critical dimension\"", "nodeType": "group", "penwidth": "4", "pos": "12688,33150", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "11.597" }, { "_gvid": 189, "name": "group1992199428", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"73 | 136 | 210\"", "frequence": "\"3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0\"", "from": "1992", "gid": "group1992199428", "height": "11.014", "label": "
FINITE-SIZE SCALING TECHNIQUES | ISING SPIN-GLASSES ( 1992 , 1994 ) (((1992,1994),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-size scaling techniques<\/TD> ising spin-glasses<\/TD> transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"transition | ising spin-glasses | finite-size scaling techniques\"", "nodeType": "group", "penwidth": "4", "pos": "30950,33150", "role": "\"3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1994-10-09\"", "strTo": "\"1994-10-09\"", "support": "1", "to": "1994", "weight": "Just 1.0", "width": "11.014" }, { "_gvid": 190, "name": "period19931995", "fontsize": "50", "from": "1993", "height": "0.875", "label": "1993 1995", "nodeType": "period", "pos": "33302,32016", "shape": "box", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "to": "1995", "width": "3.9444" }, { "_gvid": 191, "name": "group1993199520", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 5 | 30\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "1993", "gid": "group1993199520", "height": "8.7222", "label": "
THEORETICAL PREDICTIONS | SCALING ( 1993 , 1995 ) (((1993,1995),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
theoretical predictions<\/TD> scaling<\/TD> field theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | theoretical predictions | field theories\"", "nodeType": "group", "penwidth": "4", "pos": "28168,32016", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "8.7222" }, { "_gvid": 192, "name": "group1993199521", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 64 | 72 | 100 | 102 | 116 | 169\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1993", "gid": "group1993199521", "height": "10.569", "label": "
FLUCTUATIONS | SCALING ( 1993 , 1995 ) (((1993,1995),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fluctuations<\/TD> scaling<\/TD> random media<\/TD> probability distribution<\/TD><\/TR>\n
polymer<\/TD> correlation length<\/TD> replica approach<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | replica approach | correlation length | fluctuations | polymer | probability distribution | random media\"", "nodeType": "group", "penwidth": "4", "pos": "23818,32016", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "10.569" }, { "_gvid": 193, "name": "group1993199522", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 63 | 193 | 216\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1993", "gid": "group1993199522", "height": "10.639", "label": "
GLASS TRANSITION | MEAN-FIELD MODEL ( 1993 , 1995 ) (((1993,1995),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glass transition<\/TD> mean-field model<\/TD> aging<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | mean-field model | aging | glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "5063.5,32016", "role": "\"3.0 | 3.0 | 3.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "10.639" }, { "_gvid": 194, "name": "group1993199523", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"12 | 14 | 37 | 132 | 202 | 225\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "1993", "gid": "group1993199523", "height": "11.278", "label": "
OFF-EQUILIBRIUM DYNAMICS | EXPANSION ( 1993 , 1995 ) (((1993,1995),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> expansion<\/TD> asymptotic behaviour<\/TD> energy<\/TD><\/TR>\n
quenched disorder<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"asymptotic behaviour | expansion | energy | spin-glass model | quenched disorder | off-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "19550,32016", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "11.278" }, { "_gvid": 195, "name": "group1993199524", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"34 | 37 | 63 | 82 | 107 | 117 | 156 | 222 | 223 | 224\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1993", "gid": "group1993199524", "height": "12.875", "label": "
CONFIGURATIONAL ENTROPY | GIBBS FREE ( 1993 , 1995 ) (((1993,1995),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
configurational entropy<\/TD> gibbs free<\/TD> metastable states<\/TD> spin models<\/TD><\/TR>\n
complexity<\/TD> high temperature expansion<\/TD> energy<\/TD> mean-field model<\/TD><\/TR>\n
replicas<\/TD> free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"high temperature expansion | energy | mean-field model | spin models | free energy | replicas | complexity | metastable states | gibbs free | configurational entropy\"", "nodeType": "group", "penwidth": "4", "pos": "20638,32016", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "12.875" }, { "_gvid": 196, "name": "group1993199526", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 55 | 107 | 109 | 117 | 200 | 222 | 231\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1993", "gid": "group1993199526", "height": "11.486", "label": "
BRAY | PARTITION FUNCTION ( 1993 , 1995 ) (((1993,1995),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
bray<\/TD> partition function<\/TD> free energy<\/TD> metastable states<\/TD><\/TR>\n
mean-field spin glasses<\/TD> spin glasses<\/TD> sherrington-kirkpatrick model<\/TD> replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | sherrington-kirkpatrick model | free energy | partition function | replicas | mean-field spin glasses | metastable states | bray\"", "nodeType": "group", "penwidth": "4", "pos": "16474,32016", "role": "\"3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "11.486" }, { "_gvid": 197, "name": "group1993199527", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 64 | 70 | 138 | 205 | 206 | 208 | 230\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1993", "gid": "group1993199527", "height": "14.819", "label": "
LOW-TEMPERATURE PHASE | THERMODYNAMIC PROPERTIES ( 1993 , 1995 ) (((1993,1995),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
low-temperature phase<\/TD> thermodynamic properties<\/TD> josephson junctions<\/TD> d-dimensional array<\/TD><\/TR>\n
magnetic field<\/TD> spin glasses<\/TD> statistical mechanics<\/TD> replica approach<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica approach | magnetic field | statistical mechanics | d-dimensional array | josephson junctions | thermodynamic properties | low-temperature phase\"", "nodeType": "group", "penwidth": "4", "pos": "14420,32016", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "14.819" }, { "_gvid": 198, "name": "group1993199528", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 64 | 83 | 133\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1993", "gid": "group1993199528", "height": "11.639", "label": "
SPIN GLASS THEORY | SPIN GLASSES ( 1993 , 1995 ) (((1993,1995),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glass theory<\/TD> spin glasses<\/TD> replica approach<\/TD> replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica approach | spin glass theory | replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "10680,32016", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "11.639" }, { "_gvid": 199, "name": "group1993199529", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 62 | 64 | 96 | 219 | 225 | 226 | 227 | 228 | 229\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1993", "gid": "group1993199529", "height": "13.014", "label": "
DYNAMICAL APPROACH | SELF-SIMILAR ( 1993 , 1995 ) (((1993,1995),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical approach<\/TD> self-similar<\/TD> auto-correlation<\/TD> long-range spin-glasses<\/TD><\/TR>\n
equilibrium<\/TD> order parameter<\/TD> sherrington-kirkpatrick model<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
equilibrium dynamics<\/TD> replica approach<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | order parameter | replica approach | equilibrium | equilibrium dynamics | off-equilibrium dynamics | long-range spin-glasses | auto-correlation | self-similar | dynamical approach\"", "nodeType": "group", "penwidth": "4", "pos": "8093.5,32016", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 2.0 | 2.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "13.014" }, { "_gvid": 200, "name": "group19931995210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"75 | 133 | 138\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1993", "gid": "group19931995210", "height": "11.736", "label": "
REPLICA SYMMETRY BREAKING | REPLICA SYMMETRY ( 1993 , 1995 ) (((1993,1995),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica symmetry breaking<\/TD> replica symmetry<\/TD> statistical mechanics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica symmetry | replica symmetry breaking | statistical mechanics\"", "nodeType": "group", "penwidth": "4", "pos": "9484.5,32016", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1995-10-09\"", "strTo": "\"1995-10-09\"", "support": "1", "to": "1995", "weight": "Just 1.0", "width": "11.736" }, { "_gvid": 201, "name": "period19941996", "fontsize": "50", "from": "1994", "height": "0.875", "label": "1994 1996", "nodeType": "period", "pos": "33302,30916", "shape": "box", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "to": "1996", "width": "3.9444" }, { "_gvid": 202, "name": "group1994199620", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 5 | 53 | 76 | 97 | 234 | 242\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1994", "gid": "group1994199620", "height": "13.736", "label": "
UPPER CRITICAL DIMENSION | THEORETICAL PREDICTIONS ( 1994 , 1996 ) (((1994,1996),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
upper critical dimension<\/TD> theoretical predictions<\/TD> scaling<\/TD> binder cumulants<\/TD><\/TR>\n
ising model<\/TD> critical temperature<\/TD> mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | theoretical predictions | mean field theory | critical temperature | ising model | binder cumulants | upper critical dimension\"", "nodeType": "group", "penwidth": "4", "pos": "28168,30916", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "13.736" }, { "_gvid": 203, "name": "group1994199621", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 54 | 62 | 76 | 96 | 201 | 225\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1994", "gid": "group1994199621", "height": "10.25", "label": "
4D | EQUILIBRIUM ( 1994 , 1996 ) (((1994,1996),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
4d<\/TD> equilibrium<\/TD> order parameter<\/TD> critical temperature<\/TD><\/TR>\n
spin glasses<\/TD> critical exponents<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | spin glasses | order parameter | critical temperature | equilibrium | 4d | off-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "7515.5,30916", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "10.25" }, { "_gvid": 204, "name": "group1994199622", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 117 | 130 | 233 | 234\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1994", "gid": "group1994199622", "height": "12.833", "label": "
THREE-DIMENSIONAL ISING SPIN GLASS MODEL | ULTRAMETRICITY ( 1994 , 1996 ) (((1994,1996),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
three-dimensional ising spin glass model<\/TD> ultrametricity<\/TD> phase transition<\/TD> replicas<\/TD><\/TR>\n
binder cumulants<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | replicas | ultrametricity | three-dimensional ising spin glass model | binder cumulants\"", "nodeType": "group", "penwidth": "4", "pos": "5230.5,30916", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "12.833" }, { "_gvid": 205, "name": "group1994199623", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"16 | 37 | 55 | 59 | 237\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "1994", "gid": "group1994199623", "height": "10.944", "label": "
ZERO TEMPERATURE | ENERGY ( 1994 , 1996 ) (((1994,1996),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
zero temperature<\/TD> energy<\/TD> analytical solution<\/TD> sherrington-kirkpatrick model<\/TD><\/TR>\n
renormalization<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization | energy | sherrington-kirkpatrick model | zero temperature | analytical solution\"", "nodeType": "group", "penwidth": "4", "pos": "4302.5,30916", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "10.944" }, { "_gvid": 206, "name": "group1994199624", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"34 | 53 | 54 | 63 | 70 | 134 | 138 | 144 | 205 | 206 | 208 | 209 | 230\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1994", "gid": "group1994199624", "height": "12.903", "label": "
TRANSITION POINT | MAGNETIC FIELD ( 1994 , 1996 ) (((1994,1996),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
transition point<\/TD> magnetic field<\/TD> thermodynamic properties<\/TD> josephson junctions<\/TD><\/TR>\n
d-dimensional array<\/TD> matrix elements<\/TD> spin glasses<\/TD> low-temperature phase<\/TD><\/TR>\n
statistical mechanics<\/TD> disorder<\/TD> mean-field model<\/TD> high temperature expansion<\/TD><\/TR>\n
mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"high temperature expansion | mean field theory | spin glasses | mean-field model | magnetic field | disorder | statistical mechanics | matrix elements | d-dimensional array | josephson junctions | thermodynamic properties | transition point | low-temperature phase\"", "nodeType": "group", "penwidth": "4", "pos": "14420,30916", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "12.903" }, { "_gvid": 207, "name": "group1994199625", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 57 | 73 | 87 | 117 | 202 | 216 | 235 | 236\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1994", "gid": "group1994199625", "height": "11.25", "label": "
SOFT SPHERES | HYPERNETTED CHAIN ( 1994 , 1996 ) (((1994,1996),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
soft spheres<\/TD> hypernetted chain<\/TD> energy<\/TD> specific heat<\/TD><\/TR>\n
spin-glass phase<\/TD> transition<\/TD> quenched disorder<\/TD> replicas<\/TD><\/TR>\n
glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | specific heat | transition | spin-glass phase | replicas | quenched disorder | glass transition | hypernetted chain | soft spheres\"", "nodeType": "group", "penwidth": "4", "pos": "17366,30916", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "11.25" }, { "_gvid": 208, "name": "group1994199626", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 103 | 132 | 237\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "1994", "gid": "group1994199626", "height": "10.667", "label": "
ENERGY | ANALYTICAL SOLUTION ( 1994 , 1996 ) (((1994,1996),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
energy<\/TD> analytical solution<\/TD> exact solution<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | exact solution | spin-glass model | analytical solution\"", "nodeType": "group", "penwidth": "4", "pos": "19848,30916", "role": "\"3.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "10.667" }, { "_gvid": 209, "name": "group1994199627", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 64 | 74 | 79 | 136\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "1994", "gid": "group1994199627", "height": "11.861", "label": "
LOOP EXPANSION | INFRARED DIVERGENCES ( 1994 , 1996 ) (((1994,1996),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
loop expansion<\/TD> infrared divergences<\/TD> spin glasses<\/TD> replica approach<\/TD><\/TR>\n
ising spin-glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica approach | infrared divergences | loop expansion | ising spin-glasses\"", "nodeType": "group", "penwidth": "4", "pos": "10680,30916", "role": "\"3.0 | 3.0 | 2.0 | 1.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "11.861" }, { "_gvid": 210, "name": "group1994199628", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 133 | 136 | 238\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1994", "gid": "group1994199628", "height": "12.028", "label": "
EQUILIBRIUM BEHAVIOR | SPIN GLASSES ( 1994 , 1996 ) (((1994,1996),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
equilibrium behavior<\/TD> spin glasses<\/TD> ising spin-glasses<\/TD> replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica symmetry breaking | ising spin-glasses | equilibrium behavior\"", "nodeType": "group", "penwidth": "4", "pos": "9747.5,30916", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "12.028" }, { "_gvid": 211, "name": "group1994199629", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"61 | 239 | 240 | 241\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1994", "gid": "group1994199629", "height": "12.306", "label": "
ANNEALED APPROXIMATION | KAUFFMAN NETWORKS ( 1994 , 1996 ) (((1994,1996),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
annealed approximation<\/TD> kauffman networks<\/TD> attraction basins<\/TD> probability<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"probability | attraction basins | kauffman networks | annealed approximation\"", "nodeType": "group", "penwidth": "4", "pos": "25682,30916", "role": "\"3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "12.306" }, { "_gvid": 212, "name": "group19941996210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"100 | 132 | 133\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "1994", "gid": "group19941996210", "height": "11.681", "label": "
SPIN-GLASS MODEL | REPLICA SYMMETRY BREAKING ( 1994 , 1996 ) (((1994,1996),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass model<\/TD> replica symmetry breaking<\/TD> fluctuations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"fluctuations | spin-glass model | replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "12688,30916", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1996-10-09\"", "strTo": "\"1996-10-09\"", "support": "1", "to": "1996", "weight": "Just 1.0", "width": "11.681" }, { "_gvid": 213, "name": "period19951997", "fontsize": "50", "from": "1995", "height": "0.875", "label": "1995 1997", "nodeType": "period", "pos": "33302,29722", "shape": "box", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "to": "1997", "width": "3.9444" }, { "_gvid": 214, "name": "group1995199720", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 27\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199720", "height": "10.181", "label": "
ANOMALOUS DIMENSIONS | CRITICAL EXPONENTS ( 1995 , 1997 ) (((1995,1997),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
anomalous dimensions<\/TD> critical exponents<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | anomalous dimensions\"", "nodeType": "group", "penwidth": "4", "pos": "27678,29722", "role": "\"3.0 | 3.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "10.181" }, { "_gvid": 215, "name": "group1995199721", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 67 | 112 | 116 | 150 | 184 | 239 | 240 | 257\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199721", "height": "10.681", "label": "
POWER LAW | CRITICAL LINE ( 1995 , 1997 ) (((1995,1997),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
power law<\/TD> critical line<\/TD> universal<\/TD> scaling<\/TD><\/TR>\n
cycles<\/TD> critical points<\/TD> probability distribution<\/TD> kauffman networks<\/TD><\/TR>\n
attraction basins<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical points | universal | probability distribution | critical line | power law | attraction basins | kauffman networks | cycles\"", "nodeType": "group", "penwidth": "4", "pos": "24312,29722", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "10.681" }, { "_gvid": 216, "name": "group1995199722", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 23 | 37 | 87 | 88 | 133 | 136 | 253 | 254\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199722", "height": "12.833", "label": "
ANALYTICAL PREDICTIONS | SK MODEL ( 1995 , 1997 ) (((1995,1997),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
analytical predictions<\/TD> sk model<\/TD> correlation functions<\/TD> critical exponents<\/TD><\/TR>\n
spin-glass phase<\/TD> finite-dimensional spin glasses<\/TD> energy<\/TD> ising spin-glasses<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | correlation functions | energy | spin-glass phase | sk model | replica symmetry breaking | ising spin-glasses | analytical predictions | finite-dimensional spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "9388.5,29722", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "12.833" }, { "_gvid": 217, "name": "group1995199723", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 84 | 210 | 247 | 248\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199723", "height": "14.583", "label": "
UNIVERSALITY CLASS | SITE-DILUTED ISING MODEL ( 1995 , 1997 ) (((1995,1997),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
universality class<\/TD> site-diluted ising model<\/TD> finite-size scaling techniques<\/TD> monte carlo simulations<\/TD><\/TR>\n
critical exponents<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | monte carlo simulations | finite-size scaling techniques | site-diluted ising model | universality class\"", "nodeType": "group", "penwidth": "4", "pos": "30092,29722", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "14.583" }, { "_gvid": 218, "name": "group1995199724", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 14 | 49 | 109\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "1995", "gid": "group1995199724", "height": "8.7222", "label": "
GAS | EXPANSION ( 1995 , 1997 ) (((1995,1997),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
gas<\/TD> expansion<\/TD> phase transition<\/TD> partition function<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | expansion | gas | partition function\"", "nodeType": "group", "penwidth": "4", "pos": "14310,29722", "role": "\"3.0 | 3.0 | 0.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "8.7222" }, { "_gvid": 219, "name": "group1995199725", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 54 | 116 | 132 | 136 | 141 | 171 | 234\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199725", "height": "10.486", "label": "
2D | FINITE-SIZE EFFECT ( 1995 , 1997 ) (((1995,1997),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
2d<\/TD> finite-size effect<\/TD> ising spin-glasses<\/TD> spin glasses<\/TD><\/TR>\n
phase transition<\/TD> probability distribution<\/TD> spin-glass model<\/TD> binder cumulants<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | spin glasses | probability distribution | spin-glass model | ising spin-glasses | finite-size effect | 2d | binder cumulants\"", "nodeType": "group", "penwidth": "4", "pos": "5230.5,29722", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "10.486" }, { "_gvid": 220, "name": "group1995199726", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"18 | 37 | 54 | 63 | 126 | 128 | 132 | 156 | 230\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199726", "height": "13.778", "label": "
OVERLAP DISTRIBUTIONS | THERMODYNAMICAL LIMIT ( 1995 , 1997 ) (((1995,1997),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
overlap distributions<\/TD> thermodynamical limit<\/TD> complexity<\/TD> mean-field model<\/TD><\/TR>\n
energy<\/TD> spin glasses<\/TD> low-temperature phase<\/TD> spherical model<\/TD><\/TR>\n
spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spherical model | energy | spin glasses | mean-field model | thermodynamical limit | overlap distributions | spin-glass model | complexity | low-temperature phase\"", "nodeType": "group", "penwidth": "4", "pos": "20440,29722", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "13.778" }, { "_gvid": 221, "name": "group1995199727", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 73 | 96 | 186 | 190 | 193 | 197 | 200 | 222 | 258 | 259\"", "frequence": "\"1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199727", "height": "11.736", "label": "
STRUCTURAL GLASSES | MULTIFURCATION ( 1995 , 1997 ) (((1995,1997),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
multifurcation<\/TD> structural glasses<\/TD> bifurcation<\/TD> free-energy landscape<\/TD><\/TR>\n
transition<\/TD> equilibrium<\/TD> energy<\/TD> equilibrium states<\/TD><\/TR>\n
mean-field spin glasses<\/TD> metastable states<\/TD> aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | transition | equilibrium | free-energy landscape | equilibrium states | aging | bifurcation | mean-field spin glasses | metastable states | structural glasses | multifurcation\"", "nodeType": "group", "penwidth": "4", "pos": "15352,29722", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "11.736" }, { "_gvid": 222, "name": "group1995199729", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 64 | 133 | 181\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group1995199729", "height": "11.639", "label": "
SPIN GLASSES | GLASSY SYSTEMS ( 1995 , 1997 ) (((1995,1997),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> glassy systems<\/TD> replica approach<\/TD> replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica approach | replica symmetry breaking | glassy systems\"", "nodeType": "group", "penwidth": "4", "pos": "10680,29722", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "11.639" }, { "_gvid": 223, "name": "group19951997210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 73 | 96 | 117 | 190 | 215 | 222 | 255 | 260\"", "frequence": "\"5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997210", "height": "11.111", "label": "
PHASE SPACE | EQUILIBRIUM STATES ( 1995 , 1997 ) (((1995,1997),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
phase space<\/TD> equilibrium states<\/TD> p-spin model<\/TD> metastable states<\/TD><\/TR>\n
dynamical transition<\/TD> transition<\/TD> spin glasses<\/TD> replicas<\/TD><\/TR>\n
equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | transition | equilibrium | replicas | equilibrium states | dynamical transition | metastable states | p-spin model | phase space\"", "nodeType": "group", "penwidth": "4", "pos": "16490,29722", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "11.111" }, { "_gvid": 224, "name": "group19951997211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 87 | 209 | 243 | 244 | 245 | 246\"", "frequence": "\"5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997211", "height": "15.361", "label": "
OFF-EQUILIBRIUM CORRELATION FUNCTIONS | THERMODYNAMIC TRANSITION ( 1995 , 1997 ) (((1995,1997),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
off-equilibrium correlation functions<\/TD> thermodynamic transition<\/TD> transition point<\/TD> spin glasses<\/TD><\/TR>\n
spin-glass phase<\/TD> binary glasses<\/TD> binary mixtures<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | spin-glass phase | transition point | thermodynamic transition | binary glasses | binary mixtures | off-equilibrium correlation functions\"", "nodeType": "group", "penwidth": "4", "pos": "21560,29722", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "15.361" }, { "_gvid": 225, "name": "group19951997212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 130 | 190 | 254\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997212", "height": "13.625", "label": "
SPIN GLASSES | FINITE-DIMENSIONAL SPIN GLASSES ( 1995 , 1997 ) (((1995,1997),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> finite-dimensional spin glasses<\/TD> equilibrium states<\/TD> ultrametricity<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | ultrametricity | equilibrium states | finite-dimensional spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "13434,29722", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "13.625" }, { "_gvid": 226, "name": "group19951997213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"58 | 72 | 193 | 244\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997213", "height": "11.292", "label": "
BINARY GLASSES | CORRELATION LENGTH ( 1995 , 1997 ) (((1995,1997),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
binary glasses<\/TD> correlation length<\/TD> computer simulations<\/TD> aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"computer simulations | correlation length | aging | binary glasses\"", "nodeType": "group", "penwidth": "4", "pos": "18708,29722", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "11.292" }, { "_gvid": 227, "name": "group19951997214", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 67 | 91 | 149 | 181 | 255 | 256\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997214", "height": "11.042", "label": "
GLASSY MODELS | PHASE DIAGRAM ( 1995 , 1997 ) (((1995,1997),2),14)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glassy models<\/TD> phase diagram<\/TD> first-order transitions<\/TD> critical points<\/TD><\/TR>\n
mean-field model<\/TD> p-spin model<\/TD> glassy systems<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | critical points | first-order transitions | phase diagram | glassy systems | p-spin model | glassy models\"", "nodeType": "group", "penwidth": "4", "pos": "25274,29722", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "11.042" }, { "_gvid": 228, "name": "group19951997215", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"96 | 132 | 133 | 245 | 251 | 252\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997215", "height": "17.431", "label": "
FRAGILE GLASSES | OFF-EQUILIBRIUM FLUCTUATION-DISSIPATION RELATIONS ( 1995 , 1997 ) (((1995,1997),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fragile glasses<\/TD> off-equilibrium fluctuation-dissipation relations<\/TD> binary mixtures<\/TD> spin-glass model<\/TD><\/TR>\n
replica symmetry breaking<\/TD> equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"equilibrium | spin-glass model | replica symmetry breaking | binary mixtures | off-equilibrium fluctuation-dissipation relations | fragile glasses\"", "nodeType": "group", "penwidth": "4", "pos": "11952,29722", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "17.431" }, { "_gvid": 229, "name": "group19951997216", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"147 | 239 | 240 | 241 | 257\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997216", "height": "11.792", "label": "
KAUFFMAN NETWORKS | ATTRACTION BASINS ( 1995 , 1997 ) (((1995,1997),2),16)<\/TD><\/TR>\n
<\/TD><\/TR>\n
kauffman networks<\/TD> attraction basins<\/TD> cycles<\/TD> annealed approximation<\/TD><\/TR>\n
asymmetric neural networks<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"asymmetric neural networks | attraction basins | kauffman networks | annealed approximation | cycles\"", "nodeType": "group", "penwidth": "4", "pos": "26598,29722", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "11.792" }, { "_gvid": 230, "name": "group19951997217", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"216 | 236 | 245\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1995", "gid": "group19951997217", "height": "9.5139", "label": "
SOFT SPHERES | GLASS TRANSITION ( 1995 , 1997 ) (((1995,1997),2),17)<\/TD><\/TR>\n
<\/TD><\/TR>\n
soft spheres<\/TD> glass transition<\/TD> binary mixtures<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"glass transition | soft spheres | binary mixtures\"", "nodeType": "group", "penwidth": "4", "pos": "19530,29722", "role": "\"3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1997-10-09\"", "strTo": "\"1997-10-09\"", "support": "1", "to": "1997", "weight": "Just 1.0", "width": "9.5139" }, { "_gvid": 231, "name": "period19961998", "fontsize": "50", "from": "1996", "height": "0.875", "label": "1996 1998", "nodeType": "period", "pos": "33302,28290", "shape": "box", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "to": "1998", "width": "3.9444" }, { "_gvid": 232, "name": "group1996199820", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 9 | 54 | 64 | 96 | 181 | 202 | 276\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199820", "height": "12.333", "label": "
STOCHASTIC STABILITY | QUENCHED DISORDER ( 1996 , 1998 ) (((1996,1998),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
stochastic stability<\/TD> quenched disorder<\/TD> spin glasses<\/TD> scaling<\/TD><\/TR>\n
replica approach<\/TD> experimental verifications<\/TD> glassy systems<\/TD> equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | experimental verifications | spin glasses | replica approach | equilibrium | glassy systems | quenched disorder | stochastic stability\"", "nodeType": "group", "penwidth": "4", "pos": "11754,28290", "role": "\"3.0 | 0.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "12.333" }, { "_gvid": 233, "name": "group1996199821", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 11 | 73 | 240\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "1996", "gid": "group1996199821", "height": "10.375", "label": "
SCALING | KAUFFMAN NETWORKS ( 1996 , 1998 ) (((1996,1998),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling<\/TD> kauffman networks<\/TD> transition<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | phase transition | transition | kauffman networks\"", "nodeType": "group", "penwidth": "4", "pos": "18676,28290", "role": "\"3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "10.375" }, { "_gvid": 234, "name": "group1996199822", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 48 | 84 | 92 | 210 | 247\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199822", "height": "12.361", "label": "
CRITICAL PROPERTIES | SCALING ( 1996 , 1998 ) (((1996,1998),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical properties<\/TD> scaling<\/TD> monte carlo simulations<\/TD> site-diluted ising model<\/TD><\/TR>\n
finite-size scaling techniques<\/TD> renormalization group<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | renormalization group | monte carlo simulations | critical properties | finite-size scaling techniques | site-diluted ising model\"", "nodeType": "group", "penwidth": "4", "pos": "28816,28290", "role": "\"3.0 | 1.0 | 3.0 | 1.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "12.361" }, { "_gvid": 235, "name": "group1996199823", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 62 | 70 | 73 | 131 | 133 | 136 | 271\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1996", "gid": "group1996199823", "height": "11.806", "label": "
TIME-REVERSAL SYMMETRY | SELF-AVERAGING ( 1996 , 1998 ) (((1996,1998),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
time-reversal symmetry<\/TD> self-averaging<\/TD> spin glasses<\/TD> magnetic field<\/TD><\/TR>\n
order parameter<\/TD> scaling<\/TD> ising spin-glasses<\/TD> transition<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | order parameter | magnetic field | transition | self-averaging | replica symmetry breaking | ising spin-glasses | time-reversal symmetry\"", "nodeType": "group", "penwidth": "4", "pos": "9902.5,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "11.806" }, { "_gvid": 236, "name": "group1996199824", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 75 | 87 | 96 | 133 | 225 | 254 | 266 | 267\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199824", "height": "16.333", "label": "
EQUILIBRIUM SIMULATIONS | FLUCTUATION-DISSIPATION THEOREM ( 1996 , 1998 ) (((1996,1998),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
equilibrium simulations<\/TD> fluctuation-dissipation theorem<\/TD> spin glasses<\/TD> finite-dimensional spin glasses<\/TD><\/TR>\n
replica symmetry breaking<\/TD> off-equilibrium dynamics<\/TD> replica symmetry<\/TD> equilibrium<\/TD><\/TR>\n
scaling<\/TD> spin-glass phase<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | replica symmetry | spin-glass phase | equilibrium | replica symmetry breaking | off-equilibrium dynamics | finite-dimensional spin glasses | fluctuation-dissipation theorem | equilibrium simulations\"", "nodeType": "group", "penwidth": "4", "pos": "8817.5,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "16.333" }, { "_gvid": 237, "name": "group1996199825", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 73 | 210 | 247 | 248\"", "frequence": "\"1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199825", "height": "13.181", "label": "
UNIVERSALITY CLASS | SITE-DILUTED ISING MODEL ( 1996 , 1998 ) (((1996,1998),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
universality class<\/TD> site-diluted ising model<\/TD> finite-size scaling techniques<\/TD> scaling<\/TD><\/TR>\n
transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | transition | finite-size scaling techniques | site-diluted ising model | universality class\"", "nodeType": "group", "penwidth": "4", "pos": "30950,28290", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "13.181" }, { "_gvid": 238, "name": "group1996199826", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 116 | 150 | 240\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199826", "height": "9.8194", "label": "
CRITICAL LINE | SCALING ( 1996 , 1998 ) (((1996,1998),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical line<\/TD> scaling<\/TD> probability distribution<\/TD> kauffman networks<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | probability distribution | critical line | kauffman networks\"", "nodeType": "group", "penwidth": "4", "pos": "24064,28290", "role": "\"3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "9.8194" }, { "_gvid": 239, "name": "group1996199827", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"5 | 37 | 87 | 94 | 96 | 222 | 258 | 262 | 263\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199827", "height": "10.764", "label": "
LOW TEMPERATURE | LARGE CLASS ( 1996 , 1998 ) (((1996,1998),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
low temperature<\/TD> large class<\/TD> metastable states<\/TD> structural glasses<\/TD><\/TR>\n
equilibrium properties<\/TD> equilibrium<\/TD> energy<\/TD> spin-glass phase<\/TD><\/TR>\n
theoretical predictions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"theoretical predictions | energy | spin-glass phase | equilibrium properties | equilibrium | metastable states | structural glasses | large class | low temperature\"", "nodeType": "group", "penwidth": "4", "pos": "15278,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "10.764" }, { "_gvid": 240, "name": "group1996199828", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 11 | 23 | 54 | 96 | 116 | 133 | 225 | 230 | 284 | 285\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199828", "height": "20.347", "label": "
THREE-DIMENSIONAL ISING SPIN GLASS | THREE-DIMENSIONAL EDWARDS-ANDERSON SPIN GLASS ( 1996 , 1998 ) (((1996,1998),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
three-dimensional ising spin glass<\/TD> three-dimensional edwards-anderson spin glass<\/TD> spin glasses<\/TD> low-temperature phase<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> replica symmetry breaking<\/TD> correlation functions<\/TD> critical exponents<\/TD><\/TR>\n
probability distribution<\/TD> equilibrium<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | phase transition | correlation functions | spin glasses | equilibrium | probability distribution | replica symmetry breaking | off-equilibrium dynamics | low-temperature phase | three-dimensional edwards-anderson spin glass | three-dimensional ising spin glass\"", "nodeType": "group", "penwidth": "4", "pos": "7424.5,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "20.347" }, { "_gvid": 241, "name": "group1996199829", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 11 | 54 | 70 | 133 | 195 | 229\"", "frequence": "\"0.0 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group1996199829", "height": "13.75", "label": "
DYNAMICAL APPROACH | FOUR-DIMENSIONAL SPIN GLASS ( 1996 , 1998 ) (((1996,1998),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical approach<\/TD> four-dimensional spin glass<\/TD> spin glasses<\/TD> magnetic field<\/TD><\/TR>\n
replica symmetry breaking<\/TD> critical exponents<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | phase transition | spin glasses | magnetic field | replica symmetry breaking | four-dimensional spin glass | dynamical approach\"", "nodeType": "group", "penwidth": "4", "pos": "3195.5,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "13.75" }, { "_gvid": 242, "name": "group19961998210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 84 | 97 | 112 | 149 | 210 | 247\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998210", "height": "14.861", "label": "
MONTE CARLO SIMULATIONS | SITE-DILUTED ISING MODEL ( 1996 , 1998 ) (((1996,1998),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
monte carlo simulations<\/TD> site-diluted ising model<\/TD> finite-size scaling techniques<\/TD> critical exponents<\/TD><\/TR>\n
universal<\/TD> ising model<\/TD> phase diagram<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | monte carlo simulations | ising model | universal | phase diagram | finite-size scaling techniques | site-diluted ising model\"", "nodeType": "group", "penwidth": "4", "pos": "29868,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "14.861" }, { "_gvid": 243, "name": "group19961998211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"18 | 107 | 132 | 283\"", "frequence": "\"0.0 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "1996", "gid": "group19961998211", "height": "10.764", "label": "
STATIONARY POINTS | FREE ENERGY ( 1996 , 1998 ) (((1996,1998),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
stationary points<\/TD> free energy<\/TD> spherical model<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spherical model | free energy | spin-glass model | stationary points\"", "nodeType": "group", "penwidth": "4", "pos": "22012,28290", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "10.764" }, { "_gvid": 244, "name": "group19961998212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 54 | 100 | 132 | 225 | 230 | 270\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998212", "height": "15.681", "label": "
FLUCTUATION DISSIPATION RELATIONS | LOW-TEMPERATURE PHASE ( 1996 , 1998 ) (((1996,1998),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fluctuation dissipation relations<\/TD> low-temperature phase<\/TD> spin glasses<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
fluctuations<\/TD> spin-glass model<\/TD> correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | spin glasses | fluctuations | spin-glass model | off-equilibrium dynamics | low-temperature phase | fluctuation dissipation relations\"", "nodeType": "group", "penwidth": "4", "pos": "14254,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "15.681" }, { "_gvid": 245, "name": "group19961998213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 55 | 88 | 193 | 278\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998213", "height": "10.458", "label": "
DYNAMICAL BEHAVIOR | ENERGY ( 1996 , 1998 ) (((1996,1998),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical behavior<\/TD> energy<\/TD> sk model<\/TD> sherrington-kirkpatrick model<\/TD><\/TR>\n
aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | sherrington-kirkpatrick model | sk model | aging | dynamical behavior\"", "nodeType": "group", "penwidth": "4", "pos": "4451.5,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "10.458" }, { "_gvid": 246, "name": "group19961998215", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 58 | 136 | 261\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "1996", "gid": "group19961998215", "height": "11.653", "label": "
PARAMAGNETIC PHASE | SPIN GLASSES ( 1996 , 1998 ) (((1996,1998),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
paramagnetic phase<\/TD> spin glasses<\/TD> ising spin-glasses<\/TD> computer simulations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | computer simulations | ising spin-glasses | paramagnetic phase\"", "nodeType": "group", "penwidth": "4", "pos": "10820,28290", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "11.653" }, { "_gvid": 247, "name": "group19961998216", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 63 | 70 | 116 | 133 | 195 | 225 | 266\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998216", "height": "15.75", "label": "
SPIN GLASSES | FLUCTUATION-DISSIPATION THEOREM ( 1996 , 1998 ) (((1996,1998),2),16)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> fluctuation-dissipation theorem<\/TD> four-dimensional spin glass<\/TD> replica symmetry breaking<\/TD><\/TR>\n
magnetic field<\/TD> off-equilibrium dynamics<\/TD> probability distribution<\/TD> mean-field model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | mean-field model | magnetic field | probability distribution | replica symmetry breaking | four-dimensional spin glass | off-equilibrium dynamics | fluctuation-dissipation theorem\"", "nodeType": "group", "penwidth": "4", "pos": "6052.5,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "15.75" }, { "_gvid": 248, "name": "group19961998217", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 193 | 209 | 225 | 244 | 246\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998217", "height": "12.861", "label": "
OFF-EQUILIBRIUM CORRELATION FUNCTIONS | SPIN GLASSES ( 1996 , 1998 ) (((1996,1998),2),17)<\/TD><\/TR>\n
<\/TD><\/TR>\n
off-equilibrium correlation functions<\/TD> spin glasses<\/TD> transition point<\/TD> binary glasses<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | aging | transition point | off-equilibrium dynamics | binary glasses | off-equilibrium correlation functions\"", "nodeType": "group", "penwidth": "4", "pos": "20750,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "12.861" }, { "_gvid": 249, "name": "group19961998218", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"61 | 73 | 147 | 239 | 257\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998218", "height": "12.319", "label": "
CYCLES | ASYMMETRIC NEURAL NETWORKS ( 1996 , 1998 ) (((1996,1998),2),18)<\/TD><\/TR>\n
<\/TD><\/TR>\n
cycles<\/TD> asymmetric neural networks<\/TD> attraction basins<\/TD> probability<\/TD><\/TR>\n
transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"probability | transition | asymmetric neural networks | attraction basins | cycles\"", "nodeType": "group", "penwidth": "4", "pos": "27562,28290", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "12.319" }, { "_gvid": 250, "name": "group19961998219", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"62 | 94 | 96 | 100 | 133 | 193 | 211 | 225 | 262 | 279\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998219", "height": "14.639", "label": "
FINITE-DIMENSIONAL SYSTEMS | SHORT-RANGE INTERACTION ( 1996 , 1998 ) (((1996,1998),2),19)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-dimensional systems<\/TD> short-range interaction<\/TD> large class<\/TD> equilibrium<\/TD><\/TR>\n
equilibrium properties<\/TD> order parameter<\/TD> fluctuations<\/TD> replica symmetry breaking<\/TD><\/TR>\n
aging<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"order parameter | equilibrium properties | equilibrium | fluctuations | replica symmetry breaking | aging | short-range interaction | off-equilibrium dynamics | large class | finite-dimensional systems\"", "nodeType": "group", "penwidth": "4", "pos": "12798,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "14.639" }, { "_gvid": 251, "name": "group19961998220", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 149 | 181\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998220", "height": "9.7361", "label": "
PHASE DIAGRAM | GLASSY SYSTEMS ( 1996 , 1998 ) (((1996,1998),2),20)<\/TD><\/TR>\n
<\/TD><\/TR>\n
phase diagram<\/TD> glassy systems<\/TD> mean-field model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | phase diagram | glassy systems\"", "nodeType": "group", "penwidth": "4", "pos": "24840,28290", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "9.7361" }, { "_gvid": 252, "name": "group19961998221", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 117 | 225 | 251\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998221", "height": "14.181", "label": "
OFF-EQUILIBRIUM FLUCTUATION-DISSIPATION RELATIONS | REPLICAS ( 1996 , 1998 ) (((1996,1998),2),21)<\/TD><\/TR>\n
<\/TD><\/TR>\n
off-equilibrium fluctuation-dissipation relations<\/TD> replicas<\/TD> replica approach<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | replicas | off-equilibrium dynamics | off-equilibrium fluctuation-dissipation relations\"", "nodeType": "group", "penwidth": "4", "pos": "23128,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "14.181" }, { "_gvid": 253, "name": "group19961998222", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"67 | 91 | 149 | 181 | 199 | 244\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998222", "height": "10.889", "label": "
REAL REPLICAS | PHASE DIAGRAM ( 1996 , 1998 ) (((1996,1998),2),22)<\/TD><\/TR>\n
<\/TD><\/TR>\n
real replicas<\/TD> phase diagram<\/TD> first-order transitions<\/TD> critical points<\/TD><\/TR>\n
glassy systems<\/TD> binary glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical points | first-order transitions | phase diagram | glassy systems | real replicas | binary glasses\"", "nodeType": "group", "penwidth": "4", "pos": "26654,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "10.889" }, { "_gvid": 254, "name": "group19961998223", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"73 | 77 | 84 | 133 | 216 | 235 | 268 | 269\"", "frequence": "\"3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998223", "height": "15.847", "label": "
HARD SPHERES | HYPERNETTED CHAIN APPROXIMATION ( 1996 , 1998 ) (((1996,1998),2),23)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hard spheres<\/TD> hypernetted chain approximation<\/TD> hypernetted chain<\/TD> transition<\/TD><\/TR>\n
glass transition<\/TD> disordered systems<\/TD> monte carlo simulations<\/TD> replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"transition | disordered systems | monte carlo simulations | replica symmetry breaking | glass transition | hypernetted chain | hypernetted chain approximation | hard spheres\"", "nodeType": "group", "penwidth": "4", "pos": "17366,28290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "15.847" }, { "_gvid": 255, "name": "group19961998225", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"87 | 260 | 280 | 281 | 282\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1996", "gid": "group19961998225", "height": "11.667", "label": "
LENNARD-JONES SYSTEM | GLASS FORMERS ( 1996 , 1998 ) (((1996,1998),2),25)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lennard-jones system<\/TD> glass formers<\/TD> long time dynamics<\/TD> phase space<\/TD><\/TR>\n
spin-glass phase<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass phase | phase space | long time dynamics | glass formers | lennard-jones system\"", "nodeType": "group", "penwidth": "4", "pos": "16158,28290", "role": "\"3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "11.667" }, { "_gvid": 256, "name": "group19961998227", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"109 | 159 | 221 | 258 | 273 | 274 | 275\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1996", "gid": "group19961998227", "height": "12.875", "label": "
MOLECULAR DYNAMICS | POTENTIAL ENERGY ( 1996 , 1998 ) (((1996,1998),2),27)<\/TD><\/TR>\n
<\/TD><\/TR>\n
molecular dynamics<\/TD> potential energy<\/TD> potential energy landscape<\/TD> partition function<\/TD><\/TR>\n
saddle points<\/TD> local minima<\/TD> structural glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"partition function | local minima | saddle points | structural glasses | potential energy landscape | potential energy | molecular dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "25726,28290", "role": "\"3.0 | 3.0 | 1.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1998-10-09\"", "strTo": "\"1998-10-09\"", "support": "1", "to": "1998", "weight": "Just 1.0", "width": "12.875" }, { "_gvid": 257, "name": "period19971999", "fontsize": "50", "from": "1997", "height": "0.875", "label": "1997 1999", "nodeType": "period", "pos": "33302,26934", "shape": "box", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "to": "1999", "width": "3.9444" }, { "_gvid": 258, "name": "group1997199920", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 97 | 225\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199920", "height": "11.083", "label": "
ISING MODEL | CRITICAL EXPONENTS ( 1997 , 1999 ) (((1997,1999),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ising model<\/TD> critical exponents<\/TD> scaling<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | ising model | off-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "28336,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "11.083" }, { "_gvid": 259, "name": "group1997199921", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 97 | 210\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199921", "height": "11", "label": "
SCALING | FINITE-SIZE SCALING TECHNIQUES ( 1997 , 1999 ) (((1997,1999),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling<\/TD> finite-size scaling techniques<\/TD> ising model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | ising model | finite-size scaling techniques\"", "nodeType": "group", "penwidth": "4", "pos": "29426,26934", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "11" }, { "_gvid": 260, "name": "group1997199922", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 54 | 63 | 70 | 73 | 132 | 216 | 271 | 303 | 304\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199922", "height": "15.347", "label": "
EDWARDS-ANDERSON MODEL | CONTINUOUS PHASE TRANSITION ( 1997 , 1999 ) (((1997,1999),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
edwards-anderson model<\/TD> continuous phase transition<\/TD> time-reversal symmetry<\/TD> spin glasses<\/TD><\/TR>\n
magnetic field<\/TD> transition<\/TD> mean-field model<\/TD> spin-glass model<\/TD><\/TR>\n
phase transition<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | spin glasses | mean-field model | magnetic field | transition | spin-glass model | glass transition | time-reversal symmetry | continuous phase transition | edwards-anderson model\"", "nodeType": "group", "penwidth": "4", "pos": "6670.5,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "15.347" }, { "_gvid": 261, "name": "group1997199923", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 30 | 77 | 216 | 288\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199923", "height": "11.764", "label": "
EUCLIDEAN RANDOM MATRICES | FIELD THEORIES ( 1997 , 1999 ) (((1997,1999),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
euclidean random matrices<\/TD> field theories<\/TD> expansion<\/TD> disordered systems<\/TD><\/TR>\n
glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | field theories | disordered systems | glass transition | euclidean random matrices\"", "nodeType": "group", "penwidth": "4", "pos": "22804,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "11.764" }, { "_gvid": 262, "name": "group1997199924", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 53 | 54 | 102 | 107 | 133 | 170 | 183\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199924", "height": "13.028", "label": "
MEAN-FIELD SOLUTION | VARIATIONAL APPROACH ( 1997 , 1999 ) (((1997,1999),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mean-field solution<\/TD> variational approach<\/TD> polymer<\/TD> mean field theory<\/TD><\/TR>\n
expansion<\/TD> spin glasses<\/TD> free energy<\/TD> replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | mean field theory | spin glasses | polymer | free energy | replica symmetry breaking | variational approach | mean-field solution\"", "nodeType": "group", "penwidth": "4", "pos": "4559.5,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "13.028" }, { "_gvid": 263, "name": "group1997199925", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"31 | 62 | 87 | 93 | 116 | 134 | 193 | 234 | 278\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199925", "height": "11.861", "label": "
POTTS MODEL | BINDER CUMULANTS ( 1997 , 1999 ) (((1997,1999),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
potts model<\/TD> dynamical behavior<\/TD> binder cumulants<\/TD> disorder<\/TD><\/TR>\n
order parameter<\/TD> divergence<\/TD> spin-glass phase<\/TD> probability distribution<\/TD><\/TR>\n
aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"divergence | order parameter | spin-glass phase | potts model | probability distribution | disorder | aging | binder cumulants | dynamical behavior\"", "nodeType": "group", "penwidth": "4", "pos": "5527.5,26934", "role": "\"3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "11.861" }, { "_gvid": 264, "name": "group1997199926", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"31 | 63 | 72 | 92 | 216 | 255\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199926", "height": "11.667", "label": "
CRITICAL PROPERTIES | MEAN-FIELD MODEL ( 1997 , 1999 ) (((1997,1999),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical properties<\/TD> mean-field model<\/TD> p-spin model<\/TD> correlation length<\/TD><\/TR>\n
divergence<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"divergence | mean-field model | correlation length | critical properties | glass transition | p-spin model\"", "nodeType": "group", "penwidth": "4", "pos": "19204,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "11.667" }, { "_gvid": 265, "name": "group1997199928", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 62 | 96 | 100 | 107 | 129 | 130 | 181 | 193 | 211 | 225 | 276\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199928", "height": "13.5", "label": "
SHORT-RANGE INTERACTION | STOCHASTIC STABILITY ( 1997 , 1999 ) (((1997,1999),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
short-range interaction<\/TD> stochastic stability<\/TD> spin glasses<\/TD> pure states<\/TD><\/TR>\n
equilibrium<\/TD> fluctuations<\/TD> order parameter<\/TD> ultrametricity<\/TD><\/TR>\n
free energy<\/TD> aging<\/TD> glassy systems<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | order parameter | equilibrium | fluctuations | free energy | pure states | ultrametricity | glassy systems | aging | short-range interaction | off-equilibrium dynamics | stochastic stability\"", "nodeType": "group", "penwidth": "4", "pos": "11718,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "13.5" }, { "_gvid": 266, "name": "group1997199929", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 73 | 84 | 96 | 235 | 262 | 268\"", "frequence": "\"5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group1997199929", "height": "13.875", "label": "
HYPERNETTED CHAIN APPROXIMATION | HYPERNETTED CHAIN ( 1997 , 1999 ) (((1997,1999),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hypernetted chain approximation<\/TD> hypernetted chain<\/TD> transition<\/TD> monte carlo simulations<\/TD><\/TR>\n
equilibrium<\/TD> large class<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | transition | monte carlo simulations | equilibrium | hypernetted chain | large class | hypernetted chain approximation\"", "nodeType": "group", "penwidth": "4", "pos": "15554,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "13.875" }, { "_gvid": 267, "name": "group19971999210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"56 | 64 | 117 | 230\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group19971999210", "height": "11.139", "label": "
REPLICAS | REPLICA APPROACH ( 1997 , 1999 ) (((1997,1999),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replicas<\/TD> replica approach<\/TD> low-temperature phase<\/TD> internal energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"internal energy | replica approach | replicas | low-temperature phase\"", "nodeType": "group", "penwidth": "4", "pos": "25278,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "11.139" }, { "_gvid": 268, "name": "group19971999211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"61 | 134 | 255\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group19971999211", "height": "7.8472", "label": "
DISORDER | PROBABILITY ( 1997 , 1999 ) (((1997,1999),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
disorder<\/TD> probability<\/TD> p-spin model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"probability | disorder | p-spin model\"", "nodeType": "group", "penwidth": "4", "pos": "19980,26934", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "7.8472" }, { "_gvid": 269, "name": "group19971999212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 193 | 216 | 225 | 245 | 249 | 287\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group19971999212", "height": "12.542", "label": "
MODE COUPLING THEORY | LARGE SYSTEMS ( 1997 , 1999 ) (((1997,1999),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mode coupling theory<\/TD> large systems<\/TD> binary mixtures<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
aging<\/TD> glass transition<\/TD> replica approach<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | aging | glass transition | off-equilibrium dynamics | binary mixtures | large systems | mode coupling theory\"", "nodeType": "group", "penwidth": "4", "pos": "17676,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "12.542" }, { "_gvid": 270, "name": "group19971999213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"67 | 77 | 97 | 113 | 152 | 188 | 195 | 213 | 251\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group19971999213", "height": "12.264", "label": "
SLOW DYNAMICS | RANDOM FIELD ( 1997 , 1999 ) (((1997,1999),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
slow dynamics<\/TD> random field<\/TD> random-field ising model<\/TD> ferromagnets<\/TD><\/TR>\n
disordered systems<\/TD> critical points<\/TD> ising model<\/TD> four-dimensional spin glass<\/TD><\/TR>\n
off-equilibrium fluctuation-dissipation relations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical points | disordered systems | ising model | random field | ferromagnets | random-field ising model | four-dimensional spin glass | slow dynamics | off-equilibrium fluctuation-dissipation relations\"", "nodeType": "group", "penwidth": "4", "pos": "26444,26934", "role": "\"3.0 | 3.0 | 3.0 | 0.0 | 3.0 | 3.0 | 3.0 | 1.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "12.264" }, { "_gvid": 271, "name": "group19971999214", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"72 | 87 | 225 | 245\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1997", "gid": "group19971999214", "height": "12.222", "label": "
BINARY MIXTURES | SPIN-GLASS PHASE ( 1997 , 1999 ) (((1997,1999),2),14)<\/TD><\/TR>\n
<\/TD><\/TR>\n
binary mixtures<\/TD> spin-glass phase<\/TD> off-equilibrium dynamics<\/TD> correlation length<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation length | spin-glass phase | off-equilibrium dynamics | binary mixtures\"", "nodeType": "group", "penwidth": "4", "pos": "16712,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "12.222" }, { "_gvid": 272, "name": "group19971999215", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"87 | 117 | 137 | 138 | 208 | 224 | 236 | 243 | 245 | 253\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group19971999215", "height": "14.167", "label": "
THERMODYNAMIC PROPERTIES | SPIN-GLASS PHASE ( 1997 , 1999 ) (((1997,1999),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
thermodynamic properties<\/TD> spin-glass phase<\/TD> analytical predictions<\/TD> thermodynamic transition<\/TD><\/TR>\n
thermodynamics<\/TD> statistical mechanics<\/TD> soft spheres<\/TD> replicas<\/TD><\/TR>\n
configurational entropy<\/TD> binary mixtures<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass phase | replicas | thermodynamics | statistical mechanics | thermodynamic properties | configurational entropy | soft spheres | thermodynamic transition | binary mixtures | analytical predictions\"", "nodeType": "group", "penwidth": "4", "pos": "24296,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "14.167" }, { "_gvid": 273, "name": "group19971999216", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"225 | 270 | 274 | 280 | 282 | 302\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1997", "gid": "group19971999216", "height": "13.806", "label": "
SIMPLE GLASSES | LENNARD-JONES SYSTEM ( 1997 , 1999 ) (((1997,1999),2),16)<\/TD><\/TR>\n
<\/TD><\/TR>\n
simple glasses<\/TD> lennard-jones system<\/TD> long time dynamics<\/TD> fluctuation dissipation relations<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> potential energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"off-equilibrium dynamics | fluctuation dissipation relations | potential energy | long time dynamics | lennard-jones system | simple glasses\"", "nodeType": "group", "penwidth": "4", "pos": "14486,26934", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"1999-10-09\"", "strTo": "\"1999-10-09\"", "support": "1", "to": "1999", "weight": "Just 1.0", "width": "13.806" }, { "_gvid": 274, "name": "period19982000", "fontsize": "50", "from": "1998", "height": "0.875", "label": "1998 2000", "nodeType": "period", "pos": "33302,25674", "shape": "box", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "to": "2000", "width": "3.9444" }, { "_gvid": 275, "name": "group1998200020", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 167 | 242\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "1998", "gid": "group1998200020", "height": "11.958", "label": "
UPPER CRITICAL DIMENSION | SPATIAL DIMENSIONS ( 1998 , 2000 ) (((1998,2000),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
upper critical dimension<\/TD> spatial dimensions<\/TD> critical exponents<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | spatial dimensions | upper critical dimension\"", "nodeType": "group", "penwidth": "4", "pos": "28336,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "11.958" }, { "_gvid": 276, "name": "group1998200021", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 117 | 181 | 258 | 270\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200021", "height": "12.056", "label": "
SPIN GLASSES | GLASSY SYSTEMS ( 1998 , 2000 ) (((1998,2000),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> glassy systems<\/TD> fluctuation dissipation relations<\/TD> structural glasses<\/TD><\/TR>\n
scaling<\/TD> replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | replicas | glassy systems | structural glasses | fluctuation dissipation relations\"", "nodeType": "group", "penwidth": "4", "pos": "9324.5,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "12.056" }, { "_gvid": 277, "name": "group1998200022", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 23 | 54 | 72 | 76 | 184 | 225 | 246 | 263 | 266\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200022", "height": "15.319", "label": "
POWER LAW | OFF-EQUILIBRIUM CORRELATION FUNCTIONS ( 1998 , 2000 ) (((1998,2000),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
power law<\/TD> off-equilibrium correlation functions<\/TD> spin glasses<\/TD> critical temperature<\/TD><\/TR>\n
fluctuation-dissipation theorem<\/TD> off-equilibrium dynamics<\/TD> correlation functions<\/TD> critical exponents<\/TD><\/TR>\n
correlation length<\/TD> low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | correlation functions | spin glasses | correlation length | critical temperature | power law | off-equilibrium dynamics | off-equilibrium correlation functions | low temperature | fluctuation-dissipation theorem\"", "nodeType": "group", "penwidth": "4", "pos": "20232,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "15.319" }, { "_gvid": 278, "name": "group1998200023", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 23 | 54 | 113 | 117 | 129 | 133 | 229 | 278\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200023", "height": "12.764", "label": "
DYNAMICAL APPROACH | SPIN GLASSES ( 1998 , 2000 ) (((1998,2000),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical approach<\/TD> spin glasses<\/TD> pure states<\/TD> phase transition<\/TD><\/TR>\n
random field<\/TD> correlation functions<\/TD> dynamical behavior<\/TD> replica symmetry breaking<\/TD><\/TR>\n
replicas<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | correlation functions | spin glasses | random field | replicas | pure states | replica symmetry breaking | dynamical approach | dynamical behavior\"", "nodeType": "group", "penwidth": "4", "pos": "3195.5,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "12.764" }, { "_gvid": 279, "name": "group1998200024", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 53 | 167 | 194 | 235\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200024", "height": "11.139", "label": "
TOY MODEL | SPATIAL DIMENSIONS ( 1998 , 2000 ) (((1998,2000),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
toy model<\/TD> spatial dimensions<\/TD> mean field theory<\/TD> phase transition<\/TD><\/TR>\n
hypernetted chain<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | mean field theory | spatial dimensions | toy model | hypernetted chain\"", "nodeType": "group", "penwidth": "4", "pos": "23862,25674", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "11.139" }, { "_gvid": 280, "name": "group1998200025", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 54 | 75 | 109 | 204 | 216 | 263\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200025", "height": "11.708", "label": "
DISORDERED MODEL | REPLICA SYMMETRY ( 1998 , 2000 ) (((1998,2000),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
disordered model<\/TD> replica symmetry<\/TD> spin glasses<\/TD> phase transition<\/TD><\/TR>\n
partition function<\/TD> glass transition<\/TD> low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | spin glasses | replica symmetry | partition function | disordered model | glass transition | low temperature\"", "nodeType": "group", "penwidth": "4", "pos": "12636,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "11.708" }, { "_gvid": 281, "name": "group1998200026", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 57 | 60 | 64 | 73 | 117 | 230 | 243 | 306\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200026", "height": "14.028", "label": "
LENNARD-JONES BINARY MIXTURE | THERMODYNAMIC TRANSITION ( 1998 , 2000 ) (((1998,2000),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lennard-jones binary mixture<\/TD> thermodynamic transition<\/TD> phase transition<\/TD> entropy<\/TD><\/TR>\n
replica approach<\/TD> low-temperature phase<\/TD> replicas<\/TD> transition<\/TD><\/TR>\n
specific heat<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | specific heat | entropy | replica approach | transition | replicas | low-temperature phase | thermodynamic transition | lennard-jones binary mixture\"", "nodeType": "group", "penwidth": "4", "pos": "25278,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "14.028" }, { "_gvid": 282, "name": "group1998200027", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 60 | 64 | 73 | 216 | 253 | 306\"", "frequence": "\"0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200027", "height": "13.069", "label": "
LENNARD-JONES BINARY MIXTURE | PHASE TRANSITION ( 1998 , 2000 ) (((1998,2000),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lennard-jones binary mixture<\/TD> phase transition<\/TD> entropy<\/TD> analytical predictions<\/TD><\/TR>\n
replica approach<\/TD> transition<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | entropy | replica approach | transition | glass transition | analytical predictions | lennard-jones binary mixture\"", "nodeType": "group", "penwidth": "4", "pos": "17620,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "13.069" }, { "_gvid": 283, "name": "group1998200028", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 64 | 156 | 216 | 224 | 305\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200028", "height": "13.097", "label": "
THERMODYNAMIC GLASS TRANSITION | COMPLEXITY ( 1998 , 2000 ) (((1998,2000),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
thermodynamic glass transition<\/TD> complexity<\/TD> phase transition<\/TD> replica approach<\/TD><\/TR>\n
glass transition<\/TD> configurational entropy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | replica approach | complexity | glass transition | configurational entropy | thermodynamic glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "4198.5,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "13.097" }, { "_gvid": 284, "name": "group1998200029", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 36 | 54 | 116 | 133 | 142\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group1998200029", "height": "11.347", "label": "
LATTICE SIZE | SPIN GLASSES ( 1998 , 2000 ) (((1998,2000),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lattice size<\/TD> spin glasses<\/TD> replica symmetry breaking<\/TD> probability distribution<\/TD><\/TR>\n
correlation functions<\/TD> ground state<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | ground state | spin glasses | probability distribution | replica symmetry breaking | lattice size\"", "nodeType": "group", "penwidth": "4", "pos": "7424.5,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "11.347" }, { "_gvid": 285, "name": "group19982000210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"36 | 37 | 62 | 76 | 137 | 178 | 193 | 266 | 303\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group19982000210", "height": "16.236", "label": "
THERMODYNAMIC BEHAVIOUR | CONTINUOUS PHASE TRANSITION ( 1998 , 2000 ) (((1998,2000),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
thermodynamic behaviour<\/TD> continuous phase transition<\/TD> critical temperature<\/TD> order parameter<\/TD><\/TR>\n
energy<\/TD> ground state<\/TD> thermodynamics<\/TD> fluctuation-dissipation theorem<\/TD><\/TR>\n
aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground state | energy | order parameter | critical temperature | thermodynamics | thermodynamic behaviour | aging | fluctuation-dissipation theorem | continuous phase transition\"", "nodeType": "group", "penwidth": "4", "pos": "10416,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "16.236" }, { "_gvid": 286, "name": "group19982000211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"36 | 59 | 61 | 102 | 116 | 128 | 130 | 133 | 169\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group19982000211", "height": "12.222", "label": "
RANDOM MEDIA | OVERLAP DISTRIBUTIONS ( 1998 , 2000 ) (((1998,2000),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random media<\/TD> overlap distributions<\/TD> polymer<\/TD> ground state<\/TD><\/TR>\n
probability<\/TD> zero temperature<\/TD> probability distribution<\/TD> ultrametricity<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground state | zero temperature | probability | polymer | probability distribution | overlap distributions | ultrametricity | replica symmetry breaking | random media\"", "nodeType": "group", "penwidth": "4", "pos": "16200,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "12.222" }, { "_gvid": 287, "name": "group19982000212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 55 | 96 | 116 | 141 | 190 | 200\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group19982000212", "height": "12.056", "label": "
MEAN-FIELD SPIN GLASSES | FINITE-SIZE EFFECT ( 1998 , 2000 ) (((1998,2000),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mean-field spin glasses<\/TD> finite-size effect<\/TD> equilibrium states<\/TD> energy<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> probability distribution<\/TD> equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | sherrington-kirkpatrick model | equilibrium | probability distribution | finite-size effect | equilibrium states | mean-field spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "21436,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "12.056" }, { "_gvid": 288, "name": "group19982000213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 77 | 134 | 194 | 301 | 308\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1998", "gid": "group19982000213", "height": "12", "label": "
DYNAMICAL STRUCTURE FACTOR | TOY MODEL ( 1998 , 2000 ) (((1998,2000),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical structure factor<\/TD> toy model<\/TD> disordered systems<\/TD> supercooled liquid<\/TD><\/TR>\n
disorder<\/TD> energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | disordered systems | disorder | toy model | supercooled liquid | dynamical structure factor\"", "nodeType": "group", "penwidth": "4", "pos": "22958,25674", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "12" }, { "_gvid": 289, "name": "group19982000215", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 72 | 77 | 216 | 268 | 301\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1998", "gid": "group19982000215", "height": "13.972", "label": "
HYPERNETTED CHAIN APPROXIMATION | SUPERCOOLED LIQUID ( 1998 , 2000 ) (((1998,2000),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hypernetted chain approximation<\/TD> supercooled liquid<\/TD> disordered systems<\/TD> glass transition<\/TD><\/TR>\n
correlation length<\/TD> mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | correlation length | disordered systems | glass transition | hypernetted chain approximation | supercooled liquid\"", "nodeType": "group", "penwidth": "4", "pos": "18958,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "13.972" }, { "_gvid": 290, "name": "group19982000216", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"76 | 96 | 127 | 180 | 225 | 263 | 270 | 273 | 280 | 282 | 309\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group19982000216", "height": "17.653", "label": "
STOKES-EINSTEIN RELATION | STRETCHED EXPONENTIAL RELAXATION ( 1998 , 2000 ) (((1998,2000),2),16)<\/TD><\/TR>\n
<\/TD><\/TR>\n
stokes-einstein relation<\/TD> stretched exponential relaxation<\/TD> topology<\/TD> equilibrium<\/TD><\/TR>\n
lennard-jones system<\/TD> long time dynamics<\/TD> potential energy landscape<\/TD> fluctuation dissipation relations<\/TD><\/TR>\n
critical temperature<\/TD> off-equilibrium dynamics<\/TD> low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical temperature | equilibrium | topology | stretched exponential relaxation | off-equilibrium dynamics | low temperature | fluctuation dissipation relations | potential energy landscape | long time dynamics | lennard-jones system | stokes-einstein relation\"", "nodeType": "group", "penwidth": "4", "pos": "15052,25674", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "17.653" }, { "_gvid": 291, "name": "group19982000217", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"87 | 96 | 133 | 216 | 225 | 263 | 270\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group19982000217", "height": "14.819", "label": "
FLUCTUATION DISSIPATION RELATIONS | OFF-EQUILIBRIUM DYNAMICS ( 1998 , 2000 ) (((1998,2000),2),17)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fluctuation dissipation relations<\/TD> off-equilibrium dynamics<\/TD> equilibrium<\/TD> low temperature<\/TD><\/TR>\n
replica symmetry breaking<\/TD> spin-glass phase<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass phase | equilibrium | replica symmetry breaking | glass transition | off-equilibrium dynamics | low temperature | fluctuation dissipation relations\"", "nodeType": "group", "penwidth": "4", "pos": "13664,25674", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "14.819" }, { "_gvid": 292, "name": "group19982000218", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"114 | 116 | 117 | 130 | 190 | 276 | 307\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1998", "gid": "group19982000218", "height": "12.833", "label": "
REPLICA EQUIVALENCE | EQUILIBRIUM STATES ( 1998 , 2000 ) (((1998,2000),2),18)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica equivalence<\/TD> equilibrium states<\/TD> ultrametricity<\/TD> probability distribution<\/TD><\/TR>\n
stochastic stability<\/TD> replicas<\/TD> infinite volume limit<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"infinite volume limit | probability distribution | replicas | ultrametricity | equilibrium states | stochastic stability | replica equivalence\"", "nodeType": "group", "penwidth": "4", "pos": "11680,25674", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2000-10-09\"", "strTo": "\"2000-10-09\"", "support": "1", "to": "2000", "weight": "Just 1.0", "width": "12.833" }, { "_gvid": 293, "name": "period19992001", "fontsize": "50", "from": "1999", "height": "0.875", "label": "1999 2001", "nodeType": "period", "pos": "33302,24440", "shape": "box", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "to": "2001", "width": "3.9444" }, { "_gvid": 294, "name": "group1999200120", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 36 | 54 | 133\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 0.0\"", "from": "1999", "gid": "group1999200120", "height": "10.667", "label": "
REPLICA SYMMETRY BREAKING | SPIN GLASSES ( 1999 , 2001 ) (((1999,2001),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica symmetry breaking<\/TD> spin glasses<\/TD> ground state<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | ground state | spin glasses | replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "8122.5,24440", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "10.667" }, { "_gvid": 295, "name": "group1999200121", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 77 | 258 | 288 | 301 | 308 | 312\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "1999", "gid": "group1999200121", "height": "14.597", "label": "
INVERSE PARTICLE DENSITY | DISORDERED SYSTEMS ( 1999 , 2001 ) (((1999,2001),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
inverse particle density<\/TD> disordered systems<\/TD> dynamical structure factor<\/TD> euclidean random matrices<\/TD><\/TR>\n
supercooled liquid<\/TD> expansion<\/TD> structural glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | disordered systems | structural glasses | euclidean random matrices | supercooled liquid | dynamical structure factor | inverse particle density\"", "nodeType": "group", "penwidth": "4", "pos": "22606,24440", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "14.597" }, { "_gvid": 296, "name": "group1999200122", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"26 | 61 | 314 | 315\"", "frequence": "\"0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "1999", "gid": "group1999200122", "height": "11.208", "label": "
RANDOM MATCHING PROBLEMS | PROBABILITY ( 1999 , 2001 ) (((1999,2001),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random matching problems<\/TD> probability<\/TD> infinite number<\/TD> cavity method<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"infinite number | probability | random matching problems | cavity method\"", "nodeType": "group", "penwidth": "4", "pos": "13506,24440", "role": "\"3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "11.208" }, { "_gvid": 297, "name": "group1999200123", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"32 | 77 | 127 | 134 | 204 | 217 | 301 | 308 | 311 | 312\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "1999", "gid": "group1999200123", "height": "12.903", "label": "
VIBRATIONAL SPECTRUM | REAL SYSTEMS ( 1999 , 2001 ) (((1999,2001),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
vibrational spectrum<\/TD> real systems<\/TD> disordered systems<\/TD> inverse particle density<\/TD><\/TR>\n
dynamical structure factor<\/TD> supercooled liquid<\/TD> disorder<\/TD> disordered model<\/TD><\/TR>\n
topology<\/TD> perturbative expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"perturbative expansion | disordered systems | topology | disorder | disordered model | real systems | supercooled liquid | dynamical structure factor | vibrational spectrum | inverse particle density\"", "nodeType": "group", "penwidth": "4", "pos": "23668,24440", "role": "\"1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "12.903" }, { "_gvid": 298, "name": "group1999200124", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"36 | 107 | 126 | 141 | 190 | 319 | 320\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1999", "gid": "group1999200124", "height": "10.861", "label": "
CHAOS | TEMPERATURE CHAOS ( 1999 , 2001 ) (((1999,2001),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
chaos<\/TD> temperature chaos<\/TD> thermodynamical limit<\/TD> free energy<\/TD><\/TR>\n
ground state<\/TD> finite-size effect<\/TD> equilibrium states<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground state | free energy | thermodynamical limit | finite-size effect | equilibrium states | temperature chaos | chaos\"", "nodeType": "group", "penwidth": "4", "pos": "20508,24440", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "10.861" }, { "_gvid": 299, "name": "group1999200125", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 63 | 181 | 190 | 216 | 221 | 283 | 313\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1999", "gid": "group1999200125", "height": "12.375", "label": "
DYNAMIC GLASS TRANSITION | STATIONARY POINTS ( 1999 , 2001 ) (((1999,2001),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamic glass transition<\/TD> stationary points<\/TD> saddle points<\/TD> energy<\/TD><\/TR>\n
mean-field model<\/TD> equilibrium states<\/TD> glassy systems<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | mean-field model | glassy systems | equilibrium states | glass transition | saddle points | stationary points | dynamic glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "21564,24440", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "12.375" }, { "_gvid": 300, "name": "group1999200126", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"48 | 54 | 61 | 132 | 204 | 248 | 304 | 316\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1999", "gid": "group1999200126", "height": "13.111", "label": "
GAUSSIAN SPIN GLASSES | UNIVERSALITY CLASS ( 1999 , 2001 ) (((1999,2001),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
gaussian spin glasses<\/TD> universality class<\/TD> spin-glass model<\/TD> edwards-anderson model<\/TD><\/TR>\n
spin glasses<\/TD> disordered model<\/TD> probability<\/TD> renormalization group<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization group | spin glasses | probability | spin-glass model | disordered model | universality class | edwards-anderson model | gaussian spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "9108.5,24440", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "13.111" }, { "_gvid": 301, "name": "group1999200127", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 70 | 73 | 142 | 261 | 310\"", "frequence": "\"5.555555555555558e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "1999", "gid": "group1999200127", "height": "11.486", "label": "
ENERGY LANDSCAPE | PARAMAGNETIC PHASE ( 1999 , 2001 ) (((1999,2001),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
energy landscape<\/TD> paramagnetic phase<\/TD> spin glasses<\/TD> lattice size<\/TD><\/TR>\n
magnetic field<\/TD> transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | magnetic field | transition | lattice size | paramagnetic phase | energy landscape\"", "nodeType": "group", "penwidth": "4", "pos": "7106.5,24440", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "11.486" }, { "_gvid": 302, "name": "group1999200128", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 75 | 76 | 87 | 133 | 151 | 315 | 317\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2\"", "from": "1999", "gid": "group1999200128", "height": "12.417", "label": "
BETHE LATTICE | FINITE CONNECTIVITY ( 1999 , 2001 ) (((1999,2001),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
bethe lattice<\/TD> finite connectivity<\/TD> spin glasses<\/TD> replica symmetry<\/TD><\/TR>\n
cavity method<\/TD> critical temperature<\/TD> replica symmetry breaking<\/TD> spin-glass phase<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | replica symmetry | critical temperature | spin-glass phase | replica symmetry breaking | finite connectivity | cavity method | bethe lattice\"", "nodeType": "group", "penwidth": "4", "pos": "10216,24440", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "12.417" }, { "_gvid": 303, "name": "group1999200129", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 96 | 318\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0\"", "from": "1999", "gid": "group1999200129", "height": "8.9028", "label": "
PARALLEL TEMPERING | EQUILIBRIUM ( 1999 , 2001 ) (((1999,2001),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
parallel tempering<\/TD> equilibrium<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | equilibrium | parallel tempering\"", "nodeType": "group", "penwidth": "4", "pos": "14306,24440", "role": "\"3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "8.9028" }, { "_gvid": 304, "name": "group19992001210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"87 | 127 | 193 | 225 | 302\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "1999", "gid": "group19992001210", "height": "12.069", "label": "
SIMPLE GLASSES | OFF-EQUILIBRIUM DYNAMICS ( 1999 , 2001 ) (((1999,2001),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
simple glasses<\/TD> off-equilibrium dynamics<\/TD> spin-glass phase<\/TD> aging<\/TD><\/TR>\n
topology<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass phase | topology | aging | off-equilibrium dynamics | simple glasses\"", "nodeType": "group", "penwidth": "4", "pos": "17292,24440", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "12.069" }, { "_gvid": 305, "name": "group19992001211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"236 | 245 | 305\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "1999", "gid": "group19992001211", "height": "11.292", "label": "
THERMODYNAMIC GLASS TRANSITION | BINARY MIXTURES ( 1999 , 2001 ) (((1999,2001),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
thermodynamic glass transition<\/TD> binary mixtures<\/TD> soft spheres<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"soft spheres | binary mixtures | thermodynamic glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "24904,24440", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2001-10-09\"", "strTo": "\"2001-10-09\"", "support": "1", "to": "2001", "weight": "Just 1.0", "width": "11.292" }, { "_gvid": 306, "name": "period20002002", "fontsize": "50", "from": "2000", "height": "0.875", "label": "2000 2002", "nodeType": "period", "pos": "33302,23290", "shape": "box", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "to": "2002", "width": "3.9444" }, { "_gvid": 307, "name": "group2000200220", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"1 | 59 | 69 | 75 | 82 | 88 | 230 | 255 | 286\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group2000200220", "height": "13.042", "label": "
FULL REPLICA SYMMETRY BREAKING | SK MODEL ( 2000 , 2002 ) (((2000,2002),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
full replica symmetry breaking<\/TD> sk model<\/TD> spin models<\/TD> external magnetic field<\/TD><\/TR>\n
zero temperature<\/TD> symmetry breaking<\/TD> replica symmetry<\/TD> p-spin model<\/TD><\/TR>\n
low-temperature phase<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"symmetry breaking | zero temperature | external magnetic field | replica symmetry | spin models | sk model | low-temperature phase | p-spin model | full replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "8642.5,23290", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "13.042" }, { "_gvid": 308, "name": "group2000200222", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 112 | 242\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "2000", "gid": "group2000200222", "height": "9.8333", "label": "
SCALING | UPPER CRITICAL DIMENSION ( 2000 , 2002 ) (((2000,2002),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling<\/TD> upper critical dimension<\/TD> universal<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | universal | upper critical dimension\"", "nodeType": "group", "penwidth": "4", "pos": "28336,23290", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "9.8333" }, { "_gvid": 309, "name": "group2000200223", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"8 | 23 | 30 | 72 | 77 | 100 | 131 | 188\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group2000200223", "height": "12.486", "label": "
RANDOM-FIELD ISING MODEL | SELF-AVERAGING ( 2000 , 2002 ) (((2000,2002),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random-field ising model<\/TD> self-averaging<\/TD> fluctuations<\/TD> field theories<\/TD><\/TR>\n
correlation functions<\/TD> correlation length<\/TD> scale invariance<\/TD> disordered systems<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scale invariance | correlation functions | field theories | correlation length | disordered systems | fluctuations | self-averaging | random-field ising model\"", "nodeType": "group", "penwidth": "4", "pos": "24802,23290", "role": "\"0.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "12.486" }, { "_gvid": 310, "name": "group2000200224", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 15 | 73 | 182 | 216 | 263 | 288 | 323 | 324\"", "frequence": "\"0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group2000200224", "height": "12.208", "label": "
TRANSLATIONAL INVARIANCE | BOSON PEAK ( 2000 , 2002 ) (((2000,2002),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
translational invariance<\/TD> boson peak<\/TD> dynamical phase transition<\/TD> phase transition<\/TD><\/TR>\n
euclidean space<\/TD> transition<\/TD> euclidean random matrices<\/TD> glass transition<\/TD><\/TR>\n
low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | euclidean space | transition | dynamical phase transition | glass transition | low temperature | euclidean random matrices | boson peak | translational invariance\"", "nodeType": "group", "penwidth": "4", "pos": "17392,23290", "role": "\"3.0 | 0.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "12.208" }, { "_gvid": 311, "name": "group2000200225", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 31 | 54 | 55 | 59 | 75 | 107 | 133 | 151 | 153 | 155 | 263 | 317 | 321 | 322\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "2000", "gid": "group2000200225", "height": "12.819", "label": "
FINITE NUMBER | INVERSE POWER ( 2000 , 2002 ) (((2000,2002),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite number<\/TD> inverse power<\/TD> fixed connectivity<\/TD> random lattices<\/TD><\/TR>\n
finite connectivity<\/TD> bethe lattice<\/TD> spin glasses<\/TD> replica symmetry<\/TD><\/TR>\n
free energy<\/TD> sherrington-kirkpatrick model<\/TD> replica symmetry breaking<\/TD> zero temperature<\/TD><\/TR>\n
divergence<\/TD> expansion<\/TD> low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | divergence | spin glasses | sherrington-kirkpatrick model | zero temperature | replica symmetry | free energy | replica symmetry breaking | finite connectivity | random lattices | fixed connectivity | low temperature | bethe lattice | inverse power | finite number\"", "nodeType": "group", "penwidth": "4", "pos": "9645.5,23290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "12.819" }, { "_gvid": 312, "name": "group2000200226", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 72 | 73 | 76 | 255 | 258 | 268 | 326\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group2000200226", "height": "15.375", "label": "
GLASS-FORMING LIQUIDS | HYPERNETTED CHAIN APPROXIMATION ( 2000 , 2002 ) (((2000,2002),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glass-forming liquids<\/TD> hypernetted chain approximation<\/TD> correlation length<\/TD> p-spin model<\/TD><\/TR>\n
correlation functions<\/TD> critical temperature<\/TD> transition<\/TD> structural glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | correlation length | transition | critical temperature | p-spin model | structural glasses | hypernetted chain approximation | glass-forming liquids\"", "nodeType": "group", "penwidth": "4", "pos": "18458,23290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "15.375" }, { "_gvid": 313, "name": "group2000200227", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"32 | 127 | 134 | 217 | 288 | 308 | 312\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group2000200227", "height": "12.903", "label": "
REAL SYSTEMS | INVERSE PARTICLE DENSITY ( 2000 , 2002 ) (((2000,2002),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
real systems<\/TD> inverse particle density<\/TD> disorder<\/TD> topology<\/TD><\/TR>\n
perturbative expansion<\/TD> dynamical structure factor<\/TD> euclidean random matrices<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"perturbative expansion | topology | disorder | real systems | euclidean random matrices | dynamical structure factor | inverse particle density\"", "nodeType": "group", "penwidth": "4", "pos": "23286,23290", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "12.903" }, { "_gvid": 314, "name": "group2000200228", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"36 | 54 | 225\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0\"", "from": "2000", "gid": "group2000200228", "height": "10.792", "label": "
SPIN GLASSES | OFF-EQUILIBRIUM DYNAMICS ( 2000 , 2002 ) (((2000,2002),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> off-equilibrium dynamics<\/TD> ground state<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground state | spin glasses | off-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "10714,23290", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "10.792" }, { "_gvid": 315, "name": "group2000200229", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 73 | 159 | 216 | 221 | 273 | 274 | 313\"", "frequence": "\"1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group2000200229", "height": "12.431", "label": "
POTENTIAL ENERGY | SADDLE POINTS ( 2000 , 2002 ) (((2000,2002),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
potential energy<\/TD> saddle points<\/TD> dynamic glass transition<\/TD> energy<\/TD><\/TR>\n
local minima<\/TD> transition<\/TD> glass transition<\/TD> potential energy landscape<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | transition | local minima | glass transition | saddle points | potential energy landscape | potential energy | dynamic glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "25770,23290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "2", "to": "2002", "weight": "Just 2.0", "width": "12.431" }, { "_gvid": 316, "name": "group20002002210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 127 | 193 | 225 | 273 | 310\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group20002002210", "height": "12.278", "label": "
ENERGY LANDSCAPE | POTENTIAL ENERGY LANDSCAPE ( 2000 , 2002 ) (((2000,2002),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
energy landscape<\/TD> potential energy landscape<\/TD> aging<\/TD> topology<\/TD><\/TR>\n
energy<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | topology | aging | off-equilibrium dynamics | potential energy landscape | energy landscape\"", "nodeType": "group", "penwidth": "4", "pos": "15570,23290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "12.278" }, { "_gvid": 317, "name": "group20002002211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 73 | 181 | 216 | 258 | 260 | 327\"", "frequence": "\"5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2000", "gid": "group20002002211", "height": "11.111", "label": "
KOB-ANDERSEN MODEL | PHASE SPACE ( 2000 , 2002 ) (((2000,2002),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
kob-andersen model<\/TD> phase space<\/TD> glassy systems<\/TD> spin glasses<\/TD><\/TR>\n
transition<\/TD> structural glasses<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | transition | glassy systems | glass transition | structural glasses | phase space | kob-andersen model\"", "nodeType": "group", "penwidth": "4", "pos": "6223.5,23290", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2002-10-09\"", "strTo": "\"2002-10-09\"", "support": "1", "to": "2002", "weight": "Just 1.0", "width": "11.111" }, { "_gvid": 318, "name": "period20012003", "fontsize": "50", "from": "2001", "height": "0.875", "label": "2001 2003", "nodeType": "period", "pos": "33302,22109", "shape": "box", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "to": "2003", "width": "3.9444" }, { "_gvid": 319, "name": "group2001200320", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 23 | 54 | 130 | 184 | 193 | 304 | 331 | 332\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2001", "gid": "group2001200320", "height": "13.431", "label": "
OUT-OF-EQUILIBRIUM DYNAMICS | INFINITE DIMENSIONS ( 2001 , 2003 ) (((2001,2003),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
out-of-equilibrium dynamics<\/TD> infinite dimensions<\/TD> power law<\/TD> ultrametricity<\/TD><\/TR>\n
spin glasses<\/TD> edwards-anderson model<\/TD> scaling<\/TD> correlation functions<\/TD><\/TR>\n
aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | correlation functions | spin glasses | ultrametricity | power law | aging | edwards-anderson model | infinite dimensions | out-of-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "3195.5,22109", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "13.431" }, { "_gvid": 320, "name": "group2001200321", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 37 | 67 | 73 | 112 | 159 | 274 | 283 | 301 | 323 | 334 | 335 | 336\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2001", "gid": "group2001200321", "height": "10.931", "label": "
VIBRATIONAL DENSITY | PHONONS ( 2001 , 2003 ) (((2001,2003),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
vibrational density<\/TD> phonons<\/TD> amorphous solids<\/TD> energy<\/TD><\/TR>\n
transition<\/TD> potential energy<\/TD> local minima<\/TD> stationary points<\/TD><\/TR>\n
critical points<\/TD> phase transition<\/TD> universal<\/TD> boson peak<\/TD><\/TR>\n
supercooled liquid<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | energy | critical points | transition | universal | local minima | potential energy | stationary points | supercooled liquid | boson peak | amorphous solids | phonons | vibrational density\"", "nodeType": "group", "penwidth": "4", "pos": "23734,22109", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "10.931" }, { "_gvid": 321, "name": "group2001200322", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"36 | 37 | 54 | 59 | 133 | 156 | 190 | 315 | 317 | 333\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0\"", "from": "2001", "gid": "group2001200322", "height": "11.722", "label": "
CAVITY APPROACH | BETHE LATTICE ( 2001 , 2003 ) (((2001,2003),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
cavity approach<\/TD> bethe lattice<\/TD> energy<\/TD> replica symmetry breaking<\/TD><\/TR>\n
spin glasses<\/TD> cavity method<\/TD> equilibrium states<\/TD> ground state<\/TD><\/TR>\n
zero temperature<\/TD> complexity<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground state | energy | spin glasses | zero temperature | replica symmetry breaking | complexity | equilibrium states | cavity method | bethe lattice | cavity approach\"", "nodeType": "group", "penwidth": "4", "pos": "11170,22109", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "11.722" }, { "_gvid": 322, "name": "group2001200323", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"36 | 37 | 54 | 73 | 77 | 154 | 155 | 314 | 315 | 333\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2001", "gid": "group2001200323", "height": "12.264", "label": "
RANDOM GRAPH | CAVITY APPROACH ( 2001 , 2003 ) (((2001,2003),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random graph<\/TD> cavity approach<\/TD> fixed connectivity<\/TD> spin glasses<\/TD><\/TR>\n
energy<\/TD> ground state<\/TD> disordered systems<\/TD> random matching problems<\/TD><\/TR>\n
transition<\/TD> cavity method<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground state | energy | spin glasses | transition | disordered systems | random graph | fixed connectivity | random matching problems | cavity method | cavity approach\"", "nodeType": "group", "penwidth": "4", "pos": "13452,22109", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "2", "to": "2003", "weight": "Just 2.0", "width": "12.264" }, { "_gvid": 323, "name": "group2001200325", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 75 | 133 | 315 | 316 | 317 | 337\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "2001", "gid": "group2001200325", "height": "12.764", "label": "
METASTABLE CONFIGURATIONS | BETHE LATTICE ( 2001 , 2003 ) (((2001,2003),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
metastable configurations<\/TD> bethe lattice<\/TD> cavity method<\/TD> replica symmetry breaking<\/TD><\/TR>\n
gaussian spin glasses<\/TD> energy<\/TD> replica symmetry<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | replica symmetry | replica symmetry breaking | cavity method | gaussian spin glasses | bethe lattice | metastable configurations\"", "nodeType": "group", "penwidth": "4", "pos": "10216,22109", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "12.764" }, { "_gvid": 324, "name": "group2001200326", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 116 | 193 | 270 | 276\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2001", "gid": "group2001200326", "height": "14.917", "label": "
STOCHASTIC STABILITY | FLUCTUATION DISSIPATION RELATIONS ( 2001 , 2003 ) (((2001,2003),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
stochastic stability<\/TD> fluctuation dissipation relations<\/TD> spin glasses<\/TD> probability distribution<\/TD><\/TR>\n
aging<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | probability distribution | aging | fluctuation dissipation relations | stochastic stability\"", "nodeType": "group", "penwidth": "4", "pos": "12202,22109", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "14.917" }, { "_gvid": 325, "name": "group2001200327", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 59 | 75 | 88 | 225\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "2001", "gid": "group2001200327", "height": "11.958", "label": "
SK MODEL | ZERO TEMPERATURE ( 2001 , 2003 ) (((2001,2003),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sk model<\/TD> zero temperature<\/TD> replica symmetry<\/TD> sherrington-kirkpatrick model<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | zero temperature | replica symmetry | sk model | off-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "8875.5,22109", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "11.958" }, { "_gvid": 326, "name": "group2001200328", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 60 | 66 | 107 | 132 | 156 | 181 | 198 | 222 | 328 | 329\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2001", "gid": "group2001200328", "height": "15.417", "label": "
SUPERSYMMETRIC COMPLEXITY | SHERRINGTON-KIRKPATRICK MODEL ( 2001 , 2003 ) (((2001,2003),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
supersymmetric complexity<\/TD> sherrington-kirkpatrick model<\/TD> legendre<\/TD> free energy cost<\/TD><\/TR>\n
supersymmetry<\/TD> free energy<\/TD> metastable states<\/TD> complexity<\/TD><\/TR>\n
glassy systems<\/TD> spin-glass model<\/TD> entropy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | entropy | supersymmetry | free energy | spin-glass model | complexity | glassy systems | free energy cost | metastable states | supersymmetric complexity | legendre\"", "nodeType": "group", "penwidth": "4", "pos": "21162,22109", "role": "\"3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "15.417" }, { "_gvid": 327, "name": "group2001200329", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 66 | 88 | 107 | 109 | 117 | 133 | 156 | 231\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2001", "gid": "group2001200329", "height": "12.264", "label": "
SHERRINGTON-KIRKPATRICK MODEL | SUPERSYMMETRY ( 2001 , 2003 ) (((2001,2003),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> supersymmetry<\/TD> replicas<\/TD> partition function<\/TD><\/TR>\n
bray<\/TD> free energy<\/TD> sk model<\/TD> complexity<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | supersymmetry | sk model | free energy | partition function | replicas | replica symmetry breaking | complexity | bray\"", "nodeType": "group", "penwidth": "4", "pos": "20092,22109", "role": "\"3.0 | 1.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "12.264" }, { "_gvid": 328, "name": "group20012003210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 66 | 107 | 133 | 137 | 156 | 181 | 222 | 329 | 330\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2001", "gid": "group20012003210", "height": "14.5", "label": "
SHERRINGTON-KIRKPATRICK MODEL | LEGENDRE ( 2001 , 2003 ) (((2001,2003),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> legendre<\/TD> supersymmetry<\/TD> free energy<\/TD><\/TR>\n
complexity<\/TD> becchi-rouet-stora-tyutin supersymmetry<\/TD> metastable states<\/TD> thermodynamics<\/TD><\/TR>\n
glassy systems<\/TD> replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | supersymmetry | free energy | replica symmetry breaking | thermodynamics | complexity | glassy systems | metastable states | legendre | becchi-rouet-stora-tyutin supersymmetry\"", "nodeType": "group", "penwidth": "4", "pos": "15570,22109", "role": "\"3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "14.5" }, { "_gvid": 329, "name": "group20012003211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 66 | 156 | 221 | 231 | 241 | 330\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2001", "gid": "group20012003211", "height": "14", "label": "
ANNEALED APPROXIMATION | BRAY ( 2001 , 2003 ) (((2001,2003),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
annealed approximation<\/TD> bray<\/TD> supersymmetry<\/TD> sherrington-kirkpatrick model<\/TD><\/TR>\n
complexity<\/TD> becchi-rouet-stora-tyutin supersymmetry<\/TD> saddle points<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | supersymmetry | complexity | saddle points | bray | annealed approximation | becchi-rouet-stora-tyutin supersymmetry\"", "nodeType": "group", "penwidth": "4", "pos": "19074,22109", "role": "\"3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "14" }, { "_gvid": 330, "name": "group20012003212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"73 | 182 | 263 | 323\"", "frequence": "\"3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "2001", "gid": "group20012003212", "height": "12.458", "label": "
TRANSITION | DYNAMICAL PHASE TRANSITION ( 2001 , 2003 ) (((2001,2003),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
transition<\/TD> dynamical phase transition<\/TD> boson peak<\/TD> low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"transition | dynamical phase transition | low temperature | boson peak\"", "nodeType": "group", "penwidth": "4", "pos": "17392,22109", "role": "\"3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2003-10-09\"", "strTo": "\"2003-10-09\"", "support": "1", "to": "2003", "weight": "Just 1.0", "width": "12.458" }, { "_gvid": 331, "name": "period20022004", "fontsize": "50", "from": "2002", "height": "0.875", "label": "2002 2004", "nodeType": "period", "pos": "33302,20876", "shape": "box", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "to": "2004", "width": "3.9444" }, { "_gvid": 332, "name": "group2002200420", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 11 | 96 | 193 | 252 | 258\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200420", "height": "9.0972", "label": "
FRAGILE GLASSES | SCALING ( 2002 , 2004 ) (((2002,2004),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fragile glasses<\/TD> scaling<\/TD> equilibrium<\/TD> aging<\/TD><\/TR>\n
phase transition<\/TD> structural glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | phase transition | equilibrium | aging | fragile glasses | structural glasses\"", "nodeType": "group", "penwidth": "4", "pos": "10630,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "9.0972" }, { "_gvid": 333, "name": "group2002200421", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"5 | 11 | 37 | 112 | 127 | 134 | 221 | 283 | 301 | 323 | 335 | 336\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200421", "height": "11.403", "label": "
VIBRATIONAL DENSITY | PHONONS ( 2002 , 2004 ) (((2002,2004),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
vibrational density<\/TD> phonons<\/TD> energy<\/TD> stationary points<\/TD><\/TR>\n
universal<\/TD> phase transition<\/TD> supercooled liquid<\/TD> boson peak<\/TD><\/TR>\n
topology<\/TD> disorder<\/TD> saddle points<\/TD> theoretical predictions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"theoretical predictions | phase transition | energy | universal | topology | disorder | saddle points | stationary points | supercooled liquid | boson peak | phonons | vibrational density\"", "nodeType": "group", "penwidth": "4", "pos": "23734,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "11.403" }, { "_gvid": 334, "name": "group2002200422", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"8 | 30 | 59 | 67 | 72 | 76 | 77 | 93 | 97 | 113 | 114 | 131 | 152 | 188\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200422", "height": "12.764", "label": "
FERROMAGNETS | INFINITE VOLUME LIMIT ( 2002 , 2004 ) (((2002,2004),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ferromagnets<\/TD> infinite volume limit<\/TD> random field<\/TD> ising model<\/TD><\/TR>\n
potts model<\/TD> correlation length<\/TD> field theories<\/TD> scale invariance<\/TD><\/TR>\n
self-averaging<\/TD> disordered systems<\/TD> critical temperature<\/TD> random-field ising model<\/TD><\/TR>\n
critical points<\/TD> zero temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scale invariance | field theories | zero temperature | critical points | correlation length | critical temperature | disordered systems | potts model | ising model | random field | infinite volume limit | self-averaging | ferromagnets | random-field ising model\"", "nodeType": "group", "penwidth": "4", "pos": "26298,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "12.764" }, { "_gvid": 335, "name": "group2002200423", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 37 | 133\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2002", "gid": "group2002200423", "height": "10.875", "label": "
ENERGY | REPLICA SYMMETRY BREAKING ( 2002 , 2004 ) (((2002,2004),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
energy<\/TD> replica symmetry breaking<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | energy | replica symmetry breaking\"", "nodeType": "group", "penwidth": "4", "pos": "3788.5,20876", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "10.875" }, { "_gvid": 336, "name": "group2002200424", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 54 | 63 | 102 | 133 | 153 | 200 | 272 | 279\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200424", "height": "13.875", "label": "
RANDOM ENERGY MODEL | FINITE-DIMENSIONAL SYSTEMS ( 2002 , 2004 ) (((2002,2004),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-dimensional systems<\/TD> random energy model<\/TD> mean-field spin glasses<\/TD> spin glasses<\/TD><\/TR>\n
polymer<\/TD> random lattices<\/TD> mean-field model<\/TD> energy<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | spin glasses | mean-field model | polymer | replica symmetry breaking | random lattices | mean-field spin glasses | random energy model | finite-dimensional systems\"", "nodeType": "group", "penwidth": "4", "pos": "11562,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "13.875" }, { "_gvid": 337, "name": "group2002200425", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 55 | 66 | 107 | 126 | 196 | 222 | 241 | 283\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200425", "height": "16.847", "label": "
SHERRINGTON-KIRKPATRICK MODEL | SHERRINGTON-KIRKPATRICK SPIN GLASS ( 2002 , 2004 ) (((2002,2004),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> sherrington-kirkpatrick spin glass<\/TD> thermodynamical limit<\/TD> supersymmetry<\/TD><\/TR>\n
free energy<\/TD> annealed approximation<\/TD> metastable states<\/TD> spin glasses<\/TD><\/TR>\n
stationary points<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | sherrington-kirkpatrick model | supersymmetry | free energy | thermodynamical limit | sherrington-kirkpatrick spin glass | metastable states | annealed approximation | stationary points\"", "nodeType": "group", "penwidth": "4", "pos": "17938,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "16.847" }, { "_gvid": 338, "name": "group2002200426", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 61 | 64 | 100 | 116 | 117 | 130 | 133 | 307\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200426", "height": "11.264", "label": "
REPLICA EQUIVALENCE | SPIN GLASSES ( 2002 , 2004 ) (((2002,2004),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica equivalence<\/TD> spin glasses<\/TD> replica approach<\/TD> probability<\/TD><\/TR>\n
ultrametricity<\/TD> probability distribution<\/TD> fluctuations<\/TD> replicas<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | probability | replica approach | fluctuations | probability distribution | replicas | ultrametricity | replica symmetry breaking | replica equivalence\"", "nodeType": "group", "penwidth": "4", "pos": "15072,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "11.264" }, { "_gvid": 339, "name": "group2002200427", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 63 | 96 | 107 | 117 | 156 | 255 | 330\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200427", "height": "13.278", "label": "
BECCHI-ROUET-STORA-TYUTIN SUPERSYMMETRY | FREE ENERGY ( 2002 , 2004 ) (((2002,2004),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
becchi-rouet-stora-tyutin supersymmetry<\/TD> free energy<\/TD> spin glasses<\/TD> replicas<\/TD><\/TR>\n
complexity<\/TD> mean-field model<\/TD> equilibrium<\/TD> p-spin model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | mean-field model | equilibrium | free energy | replicas | complexity | p-spin model | becchi-rouet-stora-tyutin supersymmetry\"", "nodeType": "group", "penwidth": "4", "pos": "14116,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "13.278" }, { "_gvid": 340, "name": "group2002200428", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 66 | 96 | 107 | 156 | 202 | 222 | 286 | 329 | 330\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group2002200428", "height": "15.236", "label": "
SHERRINGTON-KIRKPATRICK MODEL | SUPERSYMMETRY ( 2002 , 2004 ) (((2002,2004),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> supersymmetry<\/TD> free energy<\/TD> complexity<\/TD><\/TR>\n
legendre<\/TD> quenched disorder<\/TD> metastable states<\/TD> becchi-rouet-stora-tyutin supersymmetry<\/TD><\/TR>\n
full replica symmetry breaking<\/TD> equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | supersymmetry | equilibrium | free energy | complexity | quenched disorder | metastable states | full replica symmetry breaking | legendre | becchi-rouet-stora-tyutin supersymmetry\"", "nodeType": "group", "penwidth": "4", "pos": "19164,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "15.236" }, { "_gvid": 341, "name": "group20022004210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"193 | 266 | 270 | 276\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group20022004210", "height": "13.194", "label": "
AGING | STOCHASTIC STABILITY ( 2002 , 2004 ) (((2002,2004),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
aging<\/TD> stochastic stability<\/TD> fluctuation dissipation relations<\/TD> fluctuation-dissipation theorem<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"aging | fluctuation-dissipation theorem | fluctuation dissipation relations | stochastic stability\"", "nodeType": "group", "penwidth": "4", "pos": "12780,20876", "role": "\"3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "13.194" }, { "_gvid": 342, "name": "group20022004211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"216 | 224 | 260 | 263 | 338 | 339\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2002", "gid": "group20022004211", "height": "12.389", "label": "
VIBRATIONAL PROPERTIES | TRANSITION PATHS ( 2002 , 2004 ) (((2002,2004),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
vibrational properties<\/TD> transition paths<\/TD> phase space<\/TD> configurational entropy<\/TD><\/TR>\n
glass transition<\/TD> low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"glass transition | configurational entropy | phase space | low temperature | transition paths | vibrational properties\"", "nodeType": "group", "penwidth": "4", "pos": "5460.5,20876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2004-10-09\"", "strTo": "\"2004-10-09\"", "support": "1", "to": "2004", "weight": "Just 1.0", "width": "12.389" }, { "_gvid": 343, "name": "period20032005", "fontsize": "50", "from": "2003", "height": "0.875", "label": "2003 2005", "nodeType": "period", "pos": "33302,19691", "shape": "box", "strFrom": "\"2005-10-09\"", "strTo": "\"2005-10-09\"", "to": "2005", "width": "3.9444" }, { "_gvid": 344, "name": "group2003200520", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"29 | 54 | 59 | 66 | 132 | 156 | 263 | 317\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 3.7037037037037056e-2\"", "from": "2003", "gid": "group2003200520", "height": "11.167", "label": "
SUPERSYMMETRY | BETHE LATTICE ( 2003 , 2005 ) (((2003,2005),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
supersymmetry<\/TD> bethe lattice<\/TD> spin-glass model<\/TD> spin glasses<\/TD><\/TR>\n
complexity<\/TD> low temperature<\/TD> zero temperature<\/TD> coupling constants<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"coupling constants | spin glasses | zero temperature | supersymmetry | spin-glass model | complexity | low temperature | bethe lattice\"", "nodeType": "group", "penwidth": "4", "pos": "13364,19691", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2005-10-09\"", "strTo": "\"2005-10-09\"", "support": "1", "to": "2005", "weight": "Just 1.0", "width": "11.167" }, { "_gvid": 345, "name": "group2003200521", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 55 | 66 | 86 | 107 | 116 | 132 | 218 | 222 | 315 | 333\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2003", "gid": "group2003200521", "height": "13.722", "label": "
EXTERNAL PERTURBATION | SUPERSYMMETRY ( 2003 , 2005 ) (((2003,2005),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
external perturbation<\/TD> supersymmetry<\/TD> sherrington-kirkpatrick model<\/TD> spin glasses<\/TD><\/TR>\n
free energy<\/TD> metastable states<\/TD> spin-glass model<\/TD> cavity approach<\/TD><\/TR>\n
probability distribution<\/TD> supersymmetry breaking<\/TD> cavity method<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | sherrington-kirkpatrick model | supersymmetry | supersymmetry breaking | free energy | probability distribution | spin-glass model | external perturbation | metastable states | cavity method | cavity approach\"", "nodeType": "group", "penwidth": "4", "pos": "17938,19691", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2005-10-09\"", "strTo": "\"2005-10-09\"", "support": "1", "to": "2005", "weight": "Just 1.0", "width": "13.722" }, { "_gvid": 346, "name": "group2003200522", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 87 | 224 | 269 | 341 | 342 | 343 | 344\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2003", "gid": "group2003200522", "height": "14.056", "label": "
AMORPHOUS PACKINGS | PAIR CORRELATION FUNCTION ( 2003 , 2005 ) (((2003,2005),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
amorphous packings<\/TD> pair correlation function<\/TD> packings<\/TD> ideal glass transition<\/TD><\/TR>\n
hard spheres<\/TD> spin-glass phase<\/TD> replica approach<\/TD> configurational entropy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | spin-glass phase | configurational entropy | hard spheres | ideal glass transition | packings | pair correlation function | amorphous packings\"", "nodeType": "group", "penwidth": "4", "pos": "19190,19691", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2005-10-09\"", "strTo": "\"2005-10-09\"", "support": "1", "to": "2005", "weight": "Just 1.0", "width": "14.056" }, { "_gvid": 347, "name": "period20042006", "fontsize": "50", "from": "2004", "height": "0.875", "label": "2004 2006", "nodeType": "period", "pos": "33302,18656", "shape": "box", "strFrom": "\"2006-10-09\"", "strTo": "\"2006-10-09\"", "to": "2006", "width": "3.9444" }, { "_gvid": 348, "name": "group2004200620", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"9 | 54 | 133 | 156 | 252 | 277\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2004", "gid": "group2004200620", "height": "12.694", "label": "
COMPLEX SYSTEMS | FRAGILE GLASSES ( 2004 , 2006 ) (((2004,2006),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
complex systems<\/TD> fragile glasses<\/TD> spin glasses<\/TD> replica symmetry breaking<\/TD><\/TR>\n
complexity<\/TD> experimental verifications<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"experimental verifications | spin glasses | replica symmetry breaking | complexity | fragile glasses | complex systems\"", "nodeType": "group", "penwidth": "4", "pos": "12308,18656", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2006-10-09\"", "strTo": "\"2006-10-09\"", "support": "1", "to": "2006", "weight": "Just 1.0", "width": "12.694" }, { "_gvid": 349, "name": "group2004200621", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 60 | 73 | 269\"", "frequence": "\"0.0 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "2004", "gid": "group2004200621", "height": "8.7778", "label": "
TRANSITION | ENTROPY ( 2004 , 2006 ) (((2004,2006),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
transition<\/TD> entropy<\/TD> phase transition<\/TD> hard spheres<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | entropy | transition | hard spheres\"", "nodeType": "group", "penwidth": "4", "pos": "18382,18656", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2006-10-09\"", "strTo": "\"2006-10-09\"", "support": "1", "to": "2006", "weight": "Just 1.0", "width": "8.7778" }, { "_gvid": 350, "name": "group2004200622", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 60 | 107 | 216 | 235 | 269 | 342 | 344\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2004", "gid": "group2004200622", "height": "11.653", "label": "
HYPERNETTED CHAIN | AMORPHOUS PACKINGS ( 2004 , 2006 ) (((2004,2006),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hypernetted chain<\/TD> amorphous packings<\/TD> packings<\/TD> hard spheres<\/TD><\/TR>\n
glass transition<\/TD> entropy<\/TD> expansion<\/TD> free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | entropy | free energy | glass transition | hypernetted chain | hard spheres | packings | amorphous packings\"", "nodeType": "group", "penwidth": "4", "pos": "19190,18656", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2006-10-09\"", "strTo": "\"2006-10-09\"", "support": "1", "to": "2006", "weight": "Just 1.0", "width": "11.653" }, { "_gvid": 351, "name": "group2004200623", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 30 | 79 | 127 | 221\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2004", "gid": "group2004200623", "height": "9.75", "label": "
LOOP EXPANSION | SADDLE POINTS ( 2004 , 2006 ) (((2004,2006),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
loop expansion<\/TD> saddle points<\/TD> topology<\/TD> field theories<\/TD><\/TR>\n
correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | field theories | loop expansion | topology | saddle points\"", "nodeType": "group", "penwidth": "4", "pos": "1715.5,18656", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2006-10-09\"", "strTo": "\"2006-10-09\"", "support": "1", "to": "2006", "weight": "Just 1.0", "width": "9.75" }, { "_gvid": 352, "name": "period20052007", "fontsize": "50", "from": "2005", "height": "0.875", "label": "2005 2007", "nodeType": "period", "pos": "33302,17622", "shape": "box", "strFrom": "\"2007-10-09\"", "strTo": "\"2007-10-09\"", "to": "2007", "width": "3.9444" }, { "_gvid": 353, "name": "group2005200720", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"9 | 54 | 78 | 83\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0\"", "from": "2005", "gid": "group2005200720", "height": "14.028", "label": "
THREE-DIMENSIONAL SYSTEMS | SPIN GLASS THEORY ( 2005 , 2007 ) (((2005,2007),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glass theory<\/TD> three-dimensional systems<\/TD> spin glasses<\/TD> experimental verifications<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"experimental verifications | spin glasses | three-dimensional systems | spin glass theory\"", "nodeType": "group", "penwidth": "4", "pos": "10016,17622", "role": "\"3.0 | 3.0 | 1.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2007-10-09\"", "strTo": "\"2007-10-09\"", "support": "1", "to": "2007", "weight": "Just 1.0", "width": "14.028" }, { "_gvid": 354, "name": "group2005200721", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 70 | 81 | 128 | 130 | 304\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2005", "gid": "group2005200721", "height": "12.569", "label": "
EDWARDS-ANDERSON MODEL | ULTRAMETRICITY ( 2005 , 2007 ) (((2005,2007),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
edwards-anderson model<\/TD> ultrametricity<\/TD> overlap distributions<\/TD> excellent agreement<\/TD><\/TR>\n
magnetic field<\/TD> spin glasses<\/TD> mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | magnetic field | excellent agreement | overlap distributions | ultrametricity | edwards-anderson model\"", "nodeType": "group", "penwidth": "4", "pos": "8986.5,17622", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2007-10-09\"", "strTo": "\"2007-10-09\"", "support": "1", "to": "2007", "weight": "Just 1.0", "width": "12.569" }, { "_gvid": 355, "name": "group2005200722", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"138 | 156 | 277\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "2005", "gid": "group2005200722", "height": "9.3194", "label": "
COMPLEX SYSTEMS | COMPLEXITY ( 2005 , 2007 ) (((2005,2007),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
complex systems<\/TD> complexity<\/TD> statistical mechanics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"statistical mechanics | complexity | complex systems\"", "nodeType": "group", "penwidth": "4", "pos": "12308,17622", "role": "\"3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2007-10-09\"", "strTo": "\"2007-10-09\"", "support": "1", "to": "2007", "weight": "Just 1.0", "width": "9.3194" }, { "_gvid": 356, "name": "period20062008", "fontsize": "50", "from": "2006", "height": "0.875", "label": "2006 2008", "nodeType": "period", "pos": "33302,16556", "shape": "box", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "to": "2008", "width": "3.9444" }, { "_gvid": 357, "name": "group2006200820", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 136 | 225 | 349\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200820", "height": "12.708", "label": "
SPIN-GLASS DYNAMICS | OFF-EQUILIBRIUM DYNAMICS ( 2006 , 2008 ) (((2006,2008),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass dynamics<\/TD> off-equilibrium dynamics<\/TD> ising spin-glasses<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | ising spin-glasses | off-equilibrium dynamics | spin-glass dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "11658,16556", "role": "\"3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "12.708" }, { "_gvid": 358, "name": "group2006200821", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"9 | 54 | 70 | 94 | 254\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200821", "height": "13.583", "label": "
EQUILIBRIUM PROPERTIES | FINITE-DIMENSIONAL SPIN GLASSES ( 2006 , 2008 ) (((2006,2008),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-dimensional spin glasses<\/TD> equilibrium properties<\/TD> magnetic field<\/TD> spin glasses<\/TD><\/TR>\n
experimental verifications<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"experimental verifications | spin glasses | magnetic field | equilibrium properties | finite-dimensional spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "9584.5,16556", "role": "\"2.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "13.583" }, { "_gvid": 359, "name": "group2006200822", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 124 | 139 | 232 | 353 | 369\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200822", "height": "10.097", "label": "
PURITY | MATRIX MODELS ( 2006 , 2008 ) (((2006,2008),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
purity<\/TD> matrix models<\/TD> bipartitions<\/TD> quantum system<\/TD><\/TR>\n
phase transition<\/TD> bipartite entanglement<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | quantum system | bipartitions | matrix models | bipartite entanglement | purity\"", "nodeType": "group", "penwidth": "4", "pos": "23360,16556", "role": "\"3.0 | 1.0 | 3.0 | 1.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "10.097" }, { "_gvid": 360, "name": "group2006200823", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 91 | 204 | 216 | 272\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200823", "height": "12.972", "label": "
RANDOM ENERGY MODEL | DISORDERED MODEL ( 2006 , 2008 ) (((2006,2008),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random energy model<\/TD> disordered model<\/TD> first-order transitions<\/TD> correlation functions<\/TD><\/TR>\n
glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | first-order transitions | disordered model | glass transition | random energy model\"", "nodeType": "group", "penwidth": "4", "pos": "17740,16556", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "12.972" }, { "_gvid": 361, "name": "group2006200824", "bId": "5", "branchId": "0 71 1 12", "fontname": "Arial", "foundation": "\"49 | 343 | 354 | 355 | 356 | 357 | 358 | 359 | 360 | 361 | 362 | 363 | 364\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200824", "height": "13.361", "label": "
DENSITY FLUCTUATIONS | CONDENSED MATTER THEORY ( 2006 , 2008 ) (((2006,2008),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
density fluctuations<\/TD> condensed matter theory<\/TD> starling flocks<\/TD> starlings<\/TD><\/TR>\n
large flocks<\/TD> flocks<\/TD> individual birds<\/TD> animal groups<\/TD><\/TR>\n
pair correlation function<\/TD> spatial structure<\/TD> gas<\/TD> birds<\/TD><\/TR>\n
collective animal behaviour<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"gas | pair correlation function | animal groups | spatial structure | large flocks | starlings | individual birds | flocks | collective animal behaviour | condensed matter theory | density fluctuations | starling flocks | birds\"", "nodeType": "group", "penwidth": "4", "pos": "31680,16556", "role": "\"2.0 | 1.0 | 0.0 | 2.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 2.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "13.361" }, { "_gvid": 362, "name": "group2006200825", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 59 | 61 | 63 | 107 | 109 | 116 | 200 | 350\"", "frequence": "\"5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200825", "height": "13.292", "label": "
LARGE DEVIATIONS | MEAN-FIELD SPIN GLASSES ( 2006 , 2008 ) (((2006,2008),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
large deviations<\/TD> mean-field spin glasses<\/TD> probability distribution<\/TD> partition function<\/TD><\/TR>\n
spin glasses<\/TD> mean-field model<\/TD> probability<\/TD> zero temperature<\/TD><\/TR>\n
free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | zero temperature | probability | mean-field model | free energy | partition function | probability distribution | mean-field spin glasses | large deviations\"", "nodeType": "group", "penwidth": "4", "pos": "13382,16556", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "13.292" }, { "_gvid": 363, "name": "group2006200826", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 61 | 63 | 87 | 132 | 133 | 184 | 321 | 322\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200826", "height": "10.653", "label": "
FINITE NUMBER | INVERSE POWER ( 2006 , 2008 ) (((2006,2008),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite number<\/TD> inverse power<\/TD> power law<\/TD> spin glasses<\/TD><\/TR>\n
spin-glass model<\/TD> spin-glass phase<\/TD> mean-field model<\/TD> probability<\/TD><\/TR>\n
replica symmetry breaking<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | probability | mean-field model | spin-glass phase | spin-glass model | replica symmetry breaking | power law | inverse power | finite number\"", "nodeType": "group", "penwidth": "4", "pos": "7609.5,16556", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "10.653" }, { "_gvid": 364, "name": "group2006200827", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 84 | 249 | 265 | 367\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2006", "gid": "group2006200827", "height": "10.083", "label": "
JANUS | LARGE SYSTEMS ( 2006 , 2008 ) (((2006,2008),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
janus<\/TD> large systems<\/TD> monte carlo simulations<\/TD> spin glasses<\/TD><\/TR>\n
statistical physics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | monte carlo simulations | large systems | statistical physics | janus\"", "nodeType": "group", "penwidth": "4", "pos": "1008.5,16556", "role": "\"3.0 | 3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "10.083" }, { "_gvid": 365, "name": "group2006200828", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"60 | 138 | 269\"", "frequence": "\"0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group2006200828", "height": "8.3333", "label": "
HARD SPHERES | ENTROPY ( 2006 , 2008 ) (((2006,2008),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hard spheres<\/TD> entropy<\/TD> statistical mechanics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"entropy | statistical mechanics | hard spheres\"", "nodeType": "group", "penwidth": "4", "pos": "18592,16556", "role": "\"3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "8.3333" }, { "_gvid": 366, "name": "group20062008210", "bId": "5", "branchId": "0 71 1 12", "fontname": "Arial", "foundation": "\"127 | 218 | 358 | 359 | 360 | 364 | 368\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group20062008210", "height": "10.861", "label": "
TOPOLOGICAL INTERACTIONS | BIRDS ( 2006 , 2008 ) (((2006,2008),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
topological interactions<\/TD> birds<\/TD> flocks<\/TD> individual birds<\/TD><\/TR>\n
collective animal behaviour<\/TD> external perturbation<\/TD> topology<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"topology | external perturbation | individual birds | flocks | collective animal behaviour | birds | topological interactions\"", "nodeType": "group", "penwidth": "4", "pos": "30736,16556", "role": "\"1.0 | 1.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "10.861" }, { "_gvid": 367, "name": "group20062008211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"129 | 139 | 353 | 366\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group20062008211", "height": "9.6528", "label": "
N QUBITS | BIPARTITIONS ( 2006 , 2008 ) (((2006,2008),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
n qubits<\/TD> bipartitions<\/TD> bipartite entanglement<\/TD> pure states<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"pure states | bipartitions | bipartite entanglement | n qubits\"", "nodeType": "group", "penwidth": "4", "pos": "24192,16556", "role": "\"3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "9.6528" }, { "_gvid": 368, "name": "group20062008212", "bId": "5", "branchId": "0 71 1 12", "fontname": "Arial", "foundation": "\"356 | 357 | 358 | 359 | 360 | 363 | 364 | 365\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2006", "gid": "group20062008212", "height": "11.875", "label": "
SPATIAL COHERENCE | STARLING FLOCKS ( 2006 , 2008 ) (((2006,2008),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spatial coherence<\/TD> starling flocks<\/TD> birds<\/TD> flocks<\/TD><\/TR>\n
individual birds<\/TD> starlings<\/TD> large flocks<\/TD> collective animal behaviour<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"large flocks | starlings | individual birds | flocks | collective animal behaviour | starling flocks | birds | spatial coherence\"", "nodeType": "group", "penwidth": "4", "pos": "32660,16556", "role": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2008-10-09\"", "strTo": "\"2008-10-09\"", "support": "1", "to": "2008", "weight": "Just 1.0", "width": "11.875" }, { "_gvid": 369, "name": "period20072009", "fontsize": "50", "from": "2007", "height": "0.875", "label": "2007 2009", "nodeType": "period", "pos": "33302,15528", "shape": "box", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "to": "2009", "width": "3.9444" }, { "_gvid": 370, "name": "group2007200920", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 73 | 76 | 87 | 93 | 216 | 318 | 367\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2007", "gid": "group2007200920", "height": "11", "label": "
PARALLEL TEMPERING | POTTS MODEL ( 2007 , 2009 ) (((2007,2009),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
parallel tempering<\/TD> potts model<\/TD> scaling<\/TD> critical temperature<\/TD><\/TR>\n
critical exponents<\/TD> transition<\/TD> glass transition<\/TD> spin-glass phase<\/TD><\/TR>\n
janus<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | transition | critical temperature | spin-glass phase | potts model | glass transition | parallel tempering | janus\"", "nodeType": "group", "penwidth": "4", "pos": "7642.5,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "11" }, { "_gvid": 371, "name": "group2007200921", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 18 | 20 | 54 | 59 | 61 | 63 | 107 | 109 | 116 | 149 | 200 | 253 | 263 | 350 | 372 | 373\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2007", "gid": "group2007200921", "height": "12.597", "label": "
SMALL DEVIATIONS | EXACT EXPRESSION ( 2007 , 2009 ) (((2007,2009),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
small deviations<\/TD> exact expression<\/TD> low temperature<\/TD> analytical predictions<\/TD><\/TR>\n
phase diagram<\/TD> probability distribution<\/TD> partition function<\/TD> mean-field spin glasses<\/TD><\/TR>\n
spin glasses<\/TD> mean-field model<\/TD> zero temperature<\/TD> large deviations<\/TD><\/TR>\n
free energy<\/TD> probability<\/TD> scaling<\/TD> high orders<\/TD><\/TR>\n
spherical model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spherical model | high orders | spin glasses | zero temperature | probability | mean-field model | free energy | partition function | probability distribution | phase diagram | mean-field spin glasses | analytical predictions | low temperature | large deviations | exact expression | small deviations\"", "nodeType": "group", "penwidth": "4", "pos": "13396,15528", "role": "\"3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "12.597" }, { "_gvid": 372, "name": "group2007200922", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 23 | 54 | 96 | 349 | 367\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2007", "gid": "group2007200922", "height": "10.319", "label": "
SPIN-GLASS DYNAMICS | SCALING ( 2007 , 2009 ) (((2007,2009),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass dynamics<\/TD> scaling<\/TD> equilibrium<\/TD> spin glasses<\/TD><\/TR>\n
janus<\/TD> correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | correlation functions | spin glasses | equilibrium | spin-glass dynamics | janus\"", "nodeType": "group", "penwidth": "4", "pos": "10494,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "10.319" }, { "_gvid": 373, "name": "group2007200923", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 37 | 54 | 62 | 67 | 72 | 76 | 136 | 225 | 367 | 374\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2007", "gid": "group2007200923", "height": "12.319", "label": "
DYNAMIC HETEROGENEITIES | SCALING ( 2007 , 2009 ) (((2007,2009),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamic heterogeneities<\/TD> scaling<\/TD> critical points<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
ising spin-glasses<\/TD> order parameter<\/TD> critical temperature<\/TD> spin glasses<\/TD><\/TR>\n
energy<\/TD> correlation length<\/TD> janus<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | energy | spin glasses | order parameter | critical points | correlation length | critical temperature | ising spin-glasses | off-equilibrium dynamics | janus | dynamic heterogeneities\"", "nodeType": "group", "penwidth": "4", "pos": "11382,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "12.319" }, { "_gvid": 374, "name": "group2007200924", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"5 | 54 | 77 | 87 | 132 | 133 | 230\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "2007", "gid": "group2007200924", "height": "12.472", "label": "
SPIN GLASSES | SPIN-GLASS MODEL ( 2007 , 2009 ) (((2007,2009),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> spin-glass model<\/TD> low-temperature phase<\/TD> replica symmetry breaking<\/TD><\/TR>\n
disordered systems<\/TD> spin-glass phase<\/TD> theoretical predictions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"theoretical predictions | spin glasses | disordered systems | spin-glass phase | spin-glass model | replica symmetry breaking | low-temperature phase\"", "nodeType": "group", "penwidth": "4", "pos": "6725.5,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "12.472" }, { "_gvid": 375, "name": "group2007200925", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 54 | 62 | 133 | 184 | 230\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2007", "gid": "group2007200925", "height": "12.972", "label": "
SPIN GLASSES | REPLICA SYMMETRY BREAKING ( 2007 , 2009 ) (((2007,2009),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> replica symmetry breaking<\/TD> low-temperature phase<\/TD> power law<\/TD><\/TR>\n
order parameter<\/TD> correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | spin glasses | order parameter | replica symmetry breaking | power law | low-temperature phase\"", "nodeType": "group", "penwidth": "4", "pos": "8577.5,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "12.972" }, { "_gvid": 376, "name": "group2007200926", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 61 | 70 | 242 | 321 | 370\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2\"", "from": "2007", "gid": "group2007200926", "height": "12.972", "label": "
SPIN-GLASS TRANSITION | UPPER CRITICAL DIMENSION ( 2007 , 2009 ) (((2007,2009),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass transition<\/TD> upper critical dimension<\/TD> spin glasses<\/TD> probability<\/TD><\/TR>\n
inverse power<\/TD> magnetic field<\/TD> mean field theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | probability | magnetic field | upper critical dimension | inverse power | spin-glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "9583.5,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "12.972" }, { "_gvid": 377, "name": "group2007200927", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 64 | 103 | 107\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "2007", "gid": "group2007200927", "height": "10.569", "label": "
EXACT SOLUTION | SPIN GLASSES ( 2007 , 2009 ) (((2007,2009),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
exact solution<\/TD> spin glasses<\/TD> replica approach<\/TD> mean field theory<\/TD><\/TR>\n
free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | replica approach | exact solution | free energy\"", "nodeType": "group", "penwidth": "4", "pos": "15156,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "10.569" }, { "_gvid": 378, "name": "group2007200928", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 87 | 96 | 137 | 138 | 269 | 342 | 344 | 375\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2007", "gid": "group2007200928", "height": "12.194", "label": "
THEORETICAL MODELS | AMORPHOUS PACKINGS ( 2007 , 2009 ) (((2007,2009),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
theoretical models<\/TD> amorphous packings<\/TD> packings<\/TD> spin-glass phase<\/TD><\/TR>\n
thermodynamics<\/TD> hard spheres<\/TD> equilibrium<\/TD> replica approach<\/TD><\/TR>\n
statistical mechanics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | spin-glass phase | equilibrium | thermodynamics | statistical mechanics | hard spheres | packings | amorphous packings | theoretical models\"", "nodeType": "group", "penwidth": "4", "pos": "18592,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "12.194" }, { "_gvid": 379, "name": "group2007200929", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"87 | 245 | 269 | 342 | 344\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2007", "gid": "group2007200929", "height": "11.333", "label": "
SPIN-GLASS PHASE | AMORPHOUS PACKINGS ( 2007 , 2009 ) (((2007,2009),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass phase<\/TD> amorphous packings<\/TD> packings<\/TD> hard spheres<\/TD><\/TR>\n
binary mixtures<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass phase | binary mixtures | hard spheres | packings | amorphous packings\"", "nodeType": "group", "penwidth": "4", "pos": "19552,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "11.333" }, { "_gvid": 380, "name": "group20072009210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"138 | 139 | 366 | 369 | 371\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2007", "gid": "group20072009210", "height": "10.056", "label": "
MULTIPARTITE ENTANGLEMENT | BIPARTITIONS ( 2007 , 2009 ) (((2007,2009),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
multipartite entanglement<\/TD> bipartitions<\/TD> purity<\/TD> n qubits<\/TD><\/TR>\n
statistical mechanics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"statistical mechanics | bipartitions | n qubits | purity | multipartite entanglement\"", "nodeType": "group", "penwidth": "4", "pos": "24192,15528", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "10.056" }, { "_gvid": 381, "name": "group20072009211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"171 | 367 | 376\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2007", "gid": "group20072009211", "height": "7.0694", "label": "
JANUS ARCHITECTURE | JANUS ( 2007 , 2009 ) (((2007,2009),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
janus architecture<\/TD> janus<\/TD> 2d<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"2d | janus | janus architecture\"", "nodeType": "group", "penwidth": "4", "pos": "1137.5,15528", "role": "\"3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2009-10-09\"", "strTo": "\"2009-10-09\"", "support": "1", "to": "2009", "weight": "Just 1.0", "width": "7.0694" }, { "_gvid": 382, "name": "period20082010", "fontsize": "50", "from": "2008", "height": "0.875", "label": "2008 2010", "nodeType": "period", "pos": "33302,14371", "shape": "box", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "to": "2010", "width": "3.9444" }, { "_gvid": 383, "name": "group2008201020", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 11 | 54 | 96 | 126 | 136 | 193 | 209 | 374\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201020", "height": "10.042", "label": "
SCALING | AGING ( 2008 , 2010 ) (((2008,2010),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling<\/TD> aging<\/TD> spin glasses<\/TD> transition point<\/TD><\/TR>\n
ising spin-glasses<\/TD> thermodynamical limit<\/TD> equilibrium<\/TD> dynamic heterogeneities<\/TD><\/TR>\n
critical exponents<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | phase transition | spin glasses | equilibrium | thermodynamical limit | ising spin-glasses | aging | transition point | dynamic heterogeneities\"", "nodeType": "group", "penwidth": "4", "pos": "11184,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "10.042" }, { "_gvid": 384, "name": "group2008201021", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 14 | 18 | 55 | 61 | 77 | 79 | 100 | 107 | 112 | 117 | 126 | 132 | 350 | 373\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201021", "height": "10.167", "label": "
UNIVERSAL | SCALING ( 2008 , 2010 ) (((2008,2010),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
universal<\/TD> scaling<\/TD> loop expansion<\/TD> small deviations<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> spherical model<\/TD> replicas<\/TD> large deviations<\/TD><\/TR>\n
free energy<\/TD> fluctuations<\/TD> probability<\/TD> expansion<\/TD><\/TR>\n
disordered systems<\/TD> spin-glass model<\/TD> thermodynamical limit<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | expansion | spherical model | sherrington-kirkpatrick model | probability | disordered systems | loop expansion | fluctuations | free energy | universal | replicas | thermodynamical limit | spin-glass model | large deviations | small deviations\"", "nodeType": "group", "penwidth": "4", "pos": "15432,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "10.167" }, { "_gvid": 385, "name": "group2008201022", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 23 | 54 | 87 | 96 | 126 | 133 | 225 | 263 | 285 | 318 | 340 | 380\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201022", "height": "17.167", "label": "
JANUS SPECIAL-PURPOSE | PROBABILITY DISTRIBUTION FUNCTION ( 2008 , 2010 ) (((2008,2010),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
janus special-purpose<\/TD> probability distribution function<\/TD> three-dimensional ising spin glass<\/TD> scaling<\/TD><\/TR>\n
spin glasses<\/TD> low temperature<\/TD> parallel tempering<\/TD> equilibrium<\/TD><\/TR>\n
thermodynamical limit<\/TD> spin-glass phase<\/TD> replica symmetry breaking<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | correlation functions | spin glasses | spin-glass phase | equilibrium | thermodynamical limit | replica symmetry breaking | off-equilibrium dynamics | low temperature | three-dimensional ising spin glass | parallel tempering | probability distribution function | janus special-purpose\"", "nodeType": "group", "penwidth": "4", "pos": "9868.5,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "17.167" }, { "_gvid": 386, "name": "group2008201023", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 26 | 54 | 63 | 193 | 200 | 225 | 304\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201023", "height": "12.806", "label": "
EDWARDS-ANDERSON MODEL | SCALING ( 2008 , 2010 ) (((2008,2010),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
edwards-anderson model<\/TD> scaling<\/TD> spin glasses<\/TD> mean-field spin glasses<\/TD><\/TR>\n
aging<\/TD> mean-field model<\/TD> off-equilibrium dynamics<\/TD> infinite number<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | infinite number | spin glasses | mean-field model | aging | mean-field spin glasses | off-equilibrium dynamics | edwards-anderson model\"", "nodeType": "group", "penwidth": "4", "pos": "12224,14371", "role": "\"3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "12.806" }, { "_gvid": 387, "name": "group2008201024", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 30 | 53 | 54 | 76 | 87 | 107 | 133 | 254\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201024", "height": "14.153", "label": "
SPIN GLASSES | FINITE-DIMENSIONAL SPIN GLASSES ( 2008 , 2010 ) (((2008,2010),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> finite-dimensional spin glasses<\/TD> scaling<\/TD> replica symmetry breaking<\/TD><\/TR>\n
critical temperature<\/TD> spin-glass phase<\/TD> free energy<\/TD> mean field theory<\/TD><\/TR>\n
field theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | field theories | mean field theory | spin glasses | critical temperature | spin-glass phase | free energy | replica symmetry breaking | finite-dimensional spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "13560,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "14.153" }, { "_gvid": 388, "name": "group2008201025", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 55 | 100 | 107 | 132 | 154 | 155 | 350 | 373\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201025", "height": "12.681", "label": "
FIXED CONNECTIVITY | SMALL DEVIATIONS ( 2008 , 2010 ) (((2008,2010),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fixed connectivity<\/TD> small deviations<\/TD> scaling<\/TD> spin glasses<\/TD><\/TR>\n
free energy<\/TD> large deviations<\/TD> sherrington-kirkpatrick model<\/TD> spin-glass model<\/TD><\/TR>\n
fluctuations<\/TD> random graph<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | sherrington-kirkpatrick model | fluctuations | free energy | spin-glass model | random graph | fixed connectivity | large deviations | small deviations\"", "nodeType": "group", "penwidth": "4", "pos": "16342,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "12.681" }, { "_gvid": 389, "name": "group2008201026", "bId": "5", "branchId": "0 71 1 12", "fontname": "Arial", "foundation": "\"4 | 100 | 354 | 356 | 357 | 358 | 359 | 360 | 363 | 364 | 381 | 382 | 383 | 384 | 385\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201026", "height": "11.708", "label": "
BIRD FLOCKS | COLLECTIVE RESPONSE ( 2008 , 2010 ) (((2008,2010),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
collective response<\/TD> environmental perturbations<\/TD> fish schools<\/TD> bird flocks<\/TD><\/TR>\n
scale-free<\/TD> starling flocks<\/TD> birds<\/TD> flocks<\/TD><\/TR>\n
individual birds<\/TD> large flocks<\/TD> starlings<\/TD> animal groups<\/TD><\/TR>\n
collective animal behaviour<\/TD> scaling<\/TD> fluctuations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | fluctuations | animal groups | large flocks | starlings | individual birds | flocks | collective animal behaviour | starling flocks | birds | scale-free | bird flocks | fish schools | environmental perturbations | collective response\"", "nodeType": "group", "penwidth": "4", "pos": "31788,14371", "role": "\"1.0 | 1.0 | 2.0 | 2.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 0.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "11.708" }, { "_gvid": 390, "name": "group2008201027", "bId": "5", "branchId": "0 71 1 12", "fontname": "Arial", "foundation": "\"4 | 127 | 354 | 360 | 363 | 364 | 375 | 379\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201027", "height": "11.458", "label": "
SELF-ORGANIZED | STARLING FLOCKS ( 2008 , 2010 ) (((2008,2010),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
self-organized<\/TD> starling flocks<\/TD> birds<\/TD> collective animal behaviour<\/TD><\/TR>\n
animal groups<\/TD> theoretical models<\/TD> scaling<\/TD> topology<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | topology | animal groups | collective animal behaviour | starling flocks | birds | theoretical models | self-organized\"", "nodeType": "group", "penwidth": "4", "pos": "30736,14371", "role": "\"1.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "11.458" }, { "_gvid": 391, "name": "group2008201028", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 20 | 31 | 48 | 54 | 72 | 77 | 204 | 377 | 378\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201028", "height": "12.917", "label": "
HIERARCHICAL SPIN GLASSES | LARGE-SCALE BEHAVIOR ( 2008 , 2010 ) (((2008,2010),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hierarchical spin glasses<\/TD> large-scale behavior<\/TD> divergence<\/TD> disordered model<\/TD><\/TR>\n
renormalization group<\/TD> disordered systems<\/TD> high orders<\/TD> critical exponents<\/TD><\/TR>\n
spin glasses<\/TD> correlation length<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | high orders | divergence | renormalization group | spin glasses | correlation length | disordered systems | disordered model | large-scale behavior | hierarchical spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "6170.5,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "12.917" }, { "_gvid": 392, "name": "group2008201029", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 73 | 87 | 93 | 101\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2008", "gid": "group2008201029", "height": "10.097", "label": "
CRITICAL BEHAVIOR | POTTS MODEL ( 2008 , 2010 ) (((2008,2010),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical behavior<\/TD> potts model<\/TD> transition<\/TD> critical exponents<\/TD><\/TR>\n
spin-glass phase<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | transition | spin-glass phase | potts model | critical behavior\"", "nodeType": "group", "penwidth": "4", "pos": "8219.5,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "10.097" }, { "_gvid": 393, "name": "group20082010210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 109 | 124 | 129 | 138 | 189 | 222 | 353 | 386\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010210", "height": "12.292", "label": "
DENSITY MATRIX | METASTABLE STATES ( 2008 , 2010 ) (((2008,2010),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
density matrix<\/TD> metastable states<\/TD> finite-size corrections<\/TD> quantum system<\/TD><\/TR>\n
phase transition<\/TD> pure states<\/TD> partition function<\/TD> statistical mechanics<\/TD><\/TR>\n
bipartite entanglement<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | partition function | quantum system | pure states | statistical mechanics | finite-size corrections | metastable states | bipartite entanglement | density matrix\"", "nodeType": "group", "penwidth": "4", "pos": "23310,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "12.292" }, { "_gvid": 394, "name": "group20082010211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 54 | 55 | 62 | 132 | 151 | 153 | 317 | 319 | 320\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010211", "height": "11.847", "label": "
CHAOS | TEMPERATURE CHAOS ( 2008 , 2010 ) (((2008,2010),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
chaos<\/TD> temperature chaos<\/TD> random lattices<\/TD> finite connectivity<\/TD><\/TR>\n
spin glasses<\/TD> sherrington-kirkpatrick model<\/TD> spin-glass model<\/TD> order parameter<\/TD><\/TR>\n
expansion<\/TD> bethe lattice<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | spin glasses | sherrington-kirkpatrick model | order parameter | spin-glass model | finite connectivity | random lattices | bethe lattice | temperature chaos | chaos\"", "nodeType": "group", "penwidth": "4", "pos": "14568,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "11.847" }, { "_gvid": 395, "name": "group20082010212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 54 | 73 | 107 | 209 | 272\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010212", "height": "10.75", "label": "
TRANSITION POINT | SPIN GLASSES ( 2008 , 2010 ) (((2008,2010),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
transition point<\/TD> spin glasses<\/TD> random energy model<\/TD> free energy<\/TD><\/TR>\n
transition<\/TD> expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | spin glasses | transition | free energy | transition point | random energy model\"", "nodeType": "group", "penwidth": "4", "pos": "4303.5,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "10.75" }, { "_gvid": 396, "name": "group20082010213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 53 | 64 | 87 | 103 | 137 | 269 | 342 | 344 | 387 | 388 | 389 | 390\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2008", "gid": "group20082010213", "height": "11.486", "label": "
COLLOIDS | GRANULAR MATERIALS ( 2008 , 2010 ) (((2008,2010),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
colloids<\/TD> granular materials<\/TD> crystals<\/TD> jamming<\/TD><\/TR>\n
packings<\/TD> thermodynamics<\/TD> replica approach<\/TD> spin-glass phase<\/TD><\/TR>\n
exact solution<\/TD> amorphous packings<\/TD> hard spheres<\/TD> mean field theory<\/TD><\/TR>\n
correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | mean field theory | replica approach | spin-glass phase | exact solution | thermodynamics | hard spheres | packings | amorphous packings | jamming | crystals | granular materials | colloids\"", "nodeType": "group", "penwidth": "4", "pos": "18522,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "11.486" }, { "_gvid": 397, "name": "group20082010214", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"30 | 48 | 54 | 77 | 113 | 152 | 377\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010214", "height": "11.194", "label": "
FERROMAGNETS | RANDOM FIELD ( 2008 , 2010 ) (((2008,2010),2),14)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ferromagnets<\/TD> random field<\/TD> large-scale behavior<\/TD> disordered systems<\/TD><\/TR>\n
renormalization group<\/TD> spin glasses<\/TD> field theories<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"field theories | renormalization group | spin glasses | disordered systems | random field | ferromagnets | large-scale behavior\"", "nodeType": "group", "penwidth": "4", "pos": "7110.5,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "11.194" }, { "_gvid": 398, "name": "group20082010215", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"34 | 109 | 138 | 139 | 366 | 369 | 371\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010215", "height": "12.403", "label": "
MULTIPARTITE ENTANGLEMENT | BIPARTITIONS ( 2008 , 2010 ) (((2008,2010),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
multipartite entanglement<\/TD> bipartitions<\/TD> purity<\/TD> n qubits<\/TD><\/TR>\n
statistical mechanics<\/TD> partition function<\/TD> high temperature expansion<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"high temperature expansion | partition function | statistical mechanics | bipartitions | n qubits | purity | multipartite entanglement\"", "nodeType": "group", "penwidth": "4", "pos": "25078,14371", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "12.403" }, { "_gvid": 399, "name": "group20082010216", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 75 | 100 | 107 | 117\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010216", "height": "10.361", "label": "
REPLICAS | REPLICA APPROACH ( 2008 , 2010 ) (((2008,2010),2),16)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replicas<\/TD> replica approach<\/TD> fluctuations<\/TD> replica symmetry<\/TD><\/TR>\n
free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | replica symmetry | fluctuations | free energy | replicas\"", "nodeType": "group", "penwidth": "4", "pos": "17244,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "10.361" }, { "_gvid": 400, "name": "group20082010217", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"124 | 139 | 369 | 371\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010217", "height": "10.194", "label": "
PURITY | BIPARTITIONS ( 2008 , 2010 ) (((2008,2010),2),17)<\/TD><\/TR>\n
<\/TD><\/TR>\n
purity<\/TD> bipartitions<\/TD> multipartite entanglement<\/TD> quantum system<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"quantum system | bipartitions | purity | multipartite entanglement\"", "nodeType": "group", "penwidth": "4", "pos": "24192,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "10.194" }, { "_gvid": 401, "name": "group20082010218", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"245 | 269 | 275 | 344\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "2008", "gid": "group20082010218", "height": "12.194", "label": "
HARD SPHERES | MOLECULAR DYNAMICS ( 2008 , 2010 ) (((2008,2010),2),18)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hard spheres<\/TD> molecular dynamics<\/TD> binary mixtures<\/TD> amorphous packings<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"binary mixtures | hard spheres | molecular dynamics | amorphous packings\"", "nodeType": "group", "penwidth": "4", "pos": "20974,14371", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2010-10-09\"", "strTo": "\"2010-10-09\"", "support": "1", "to": "2010", "weight": "Just 1.0", "width": "12.194" }, { "_gvid": 402, "name": "period20092011", "fontsize": "50", "from": "2009", "height": "0.875", "label": "2009 2011", "nodeType": "period", "pos": "33302,13102", "shape": "box", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "to": "2011", "width": "3.9444" }, { "_gvid": 403, "name": "group2009201120", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 11 | 53 | 54 | 61 | 70 | 132 | 242 | 321 | 370\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2\"", "from": "2009", "gid": "group2009201120", "height": "12.333", "label": "
INVERSE POWER | SPIN-GLASS TRANSITION ( 2009 , 2011 ) (((2009,2011),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass transition<\/TD> inverse power<\/TD> magnetic field<\/TD> upper critical dimension<\/TD><\/TR>\n
spin glasses<\/TD> probability<\/TD> mean field theory<\/TD> scaling<\/TD><\/TR>\n
spin-glass model<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | phase transition | mean field theory | spin glasses | probability | magnetic field | spin-glass model | upper critical dimension | inverse power | spin-glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "10424,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "12.333" }, { "_gvid": 404, "name": "group2009201121", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 30 | 100 | 113 | 134 | 242 | 301 | 374 | 396\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201121", "height": "12.125", "label": "
QUASI-EQUILIBRIUM | SUPERCOOLED LIQUID ( 2009 , 2011 ) (((2009,2011),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
quasi-equilibrium<\/TD> supercooled liquid<\/TD> disorder<\/TD> scaling<\/TD><\/TR>\n
random field<\/TD> field theories<\/TD> fluctuations<\/TD> upper critical dimension<\/TD><\/TR>\n
dynamic heterogeneities<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | field theories | fluctuations | random field | disorder | upper critical dimension | supercooled liquid | dynamic heterogeneities | quasi-equilibrium\"", "nodeType": "group", "penwidth": "4", "pos": "17048,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "12.125" }, { "_gvid": 405, "name": "group2009201122", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 20 | 31 | 48 | 52 | 54 | 72 | 77 | 97 | 204 | 377 | 378\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201122", "height": "12.986", "label": "
HIERARCHICAL SPIN GLASSES | DISORDERED MODEL ( 2009 , 2011 ) (((2009,2011),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hierarchical spin glasses<\/TD> disordered model<\/TD> ising model<\/TD> divergence<\/TD><\/TR>\n
renormalization group<\/TD> high orders<\/TD> critical exponents<\/TD> correlation length<\/TD><\/TR>\n
large-scale behavior<\/TD> disordered systems<\/TD> explicit example<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | high orders | divergence | renormalization group | explicit example | spin glasses | correlation length | disordered systems | ising model | disordered model | large-scale behavior | hierarchical spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "6884.5,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "12.986" }, { "_gvid": 406, "name": "group2009201123", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 63 | 101 | 136 | 202 | 258 | 352 | 395\"", "frequence": "\"0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201123", "height": "14.264", "label": "
MICROSCOPIC PROPERTIES | DISCONTINUOUS TRANSITIONS ( 2009 , 2011 ) (((2009,2011),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
microscopic properties<\/TD> discontinuous transitions<\/TD> structural glasses<\/TD> quenched disorder<\/TD><\/TR>\n
phase transition<\/TD> ising spin-glasses<\/TD> critical behavior<\/TD> mean-field model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | mean-field model | critical behavior | ising spin-glasses | quenched disorder | structural glasses | discontinuous transitions | microscopic properties\"", "nodeType": "group", "penwidth": "4", "pos": "11600,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "14.264" }, { "_gvid": 407, "name": "group2009201124", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 30 | 32 | 127 | 288\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201124", "height": "13.028", "label": "
EUCLIDEAN RANDOM MATRICES | PERTURBATIVE EXPANSION ( 2009 , 2011 ) (((2009,2011),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
euclidean random matrices<\/TD> perturbative expansion<\/TD> field theories<\/TD> expansion<\/TD><\/TR>\n
topology<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | field theories | perturbative expansion | topology | euclidean random matrices\"", "nodeType": "group", "penwidth": "4", "pos": "1715.5,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "13.028" }, { "_gvid": 408, "name": "group2009201125", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 53 | 54 | 135 | 304 | 318\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201125", "height": "12.861", "label": "
LOWER CRITICAL DIMENSION | SPIN GLASSES ( 2009 , 2011 ) (((2009,2011),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
lower critical dimension<\/TD> spin glasses<\/TD> edwards-anderson model<\/TD> mean field theory<\/TD><\/TR>\n
energy<\/TD> parallel tempering<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | mean field theory | spin glasses | lower critical dimension | edwards-anderson model | parallel tempering\"", "nodeType": "group", "penwidth": "4", "pos": "12796,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "12.861" }, { "_gvid": 409, "name": "group2009201126", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 132 | 394\"", "frequence": "\"5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0\"", "from": "2009", "gid": "group2009201126", "height": "8.4306", "label": "
GPUS | SPIN-GLASS MODEL ( 2009 , 2011 ) (((2009,2011),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
gpus<\/TD> spin-glass model<\/TD> spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | spin-glass model | gpus\"", "nodeType": "group", "penwidth": "4", "pos": "14568,13102", "role": "\"3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "8.4306" }, { "_gvid": 410, "name": "group2009201127", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"61 | 76 | 100 | 128 | 130 | 141 | 267 | 276 | 284 | 373\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201127", "height": "16.069", "label": "
THREE-DIMENSIONAL EDWARDS-ANDERSON SPIN GLASS | STOCHASTIC STABILITY ( 2009 , 2011 ) (((2009,2011),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
three-dimensional edwards-anderson spin glass<\/TD> stochastic stability<\/TD> equilibrium simulations<\/TD> finite-size effect<\/TD><\/TR>\n
ultrametricity<\/TD> overlap distributions<\/TD> probability<\/TD> fluctuations<\/TD><\/TR>\n
critical temperature<\/TD> small deviations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"probability | critical temperature | fluctuations | overlap distributions | ultrametricity | finite-size effect | equilibrium simulations | stochastic stability | three-dimensional edwards-anderson spin glass | small deviations\"", "nodeType": "group", "penwidth": "4", "pos": "15668,13102", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 3.0 | 3.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "16.069" }, { "_gvid": 411, "name": "group2009201128", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 237 | 269 | 315 | 341 | 351 | 397\"", "frequence": "\"0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201128", "height": "11.694", "label": "
JAMMING POINT | JAMMING TRANSITION ( 2009 , 2011 ) (((2009,2011),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
jamming point<\/TD> jamming transition<\/TD> ideal glass transition<\/TD> cavity method<\/TD><\/TR>\n
analytical solution<\/TD> mean-field model<\/TD> hard spheres<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | analytical solution | hard spheres | cavity method | ideal glass transition | jamming transition | jamming point\"", "nodeType": "group", "penwidth": "4", "pos": "20242,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "11.694" }, { "_gvid": 412, "name": "group2009201129", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 167 | 216 | 269 | 287 | 342\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group2009201129", "height": "12.042", "label": "
MODE COUPLING THEORY | REPLICA APPROACH ( 2009 , 2011 ) (((2009,2011),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mode coupling theory<\/TD> replica approach<\/TD> spatial dimensions<\/TD> hard spheres<\/TD><\/TR>\n
packings<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | spatial dimensions | glass transition | hard spheres | mode coupling theory | packings\"", "nodeType": "group", "penwidth": "4", "pos": "18974,13102", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "12.042" }, { "_gvid": 413, "name": "group20092011210", "bId": "5", "branchId": "0 71 1 12", "fontname": "Arial", "foundation": "\"100 | 357 | 359 | 364 | 379 | 391 | 392 | 393\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2009", "gid": "group20092011210", "height": "10.861", "label": "
LOCAL STRUCTURE | ANTIPREDATOR ( 2009 , 2011 ) (((2009,2011),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
local structure<\/TD> antipredator<\/TD> collective behaviour<\/TD> flocks<\/TD><\/TR>\n
starlings<\/TD> fluctuations<\/TD> birds<\/TD> self-organized<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"fluctuations | starlings | flocks | birds | self-organized | collective behaviour | antipredator | local structure\"", "nodeType": "group", "penwidth": "4", "pos": "31258,13102", "role": "\"3.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2011-10-09\"", "strTo": "\"2011-10-09\"", "support": "1", "to": "2011", "weight": "Just 1.0", "width": "10.861" }, { "_gvid": 414, "name": "period20102012", "fontsize": "50", "from": "2010", "height": "0.875", "label": "2010 2012", "nodeType": "period", "pos": "33302,11876", "shape": "box", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "to": "2012", "width": "3.9444" }, { "_gvid": 415, "name": "group2010201220", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 11 | 54 | 69 | 101 | 195 | 216 | 242 | 258 | 271 | 305 | 380\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group2010201220", "height": "16", "label": "
THERMODYNAMIC GLASS TRANSITION | TIME-REVERSAL SYMMETRY ( 2010 , 2012 ) (((2010,2012),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
thermodynamic glass transition<\/TD> time-reversal symmetry<\/TD> four-dimensional spin glass<\/TD> scaling<\/TD><\/TR>\n
external magnetic field<\/TD> spin glasses<\/TD> phase transition<\/TD> janus special-purpose<\/TD><\/TR>\n
critical behavior<\/TD> structural glasses<\/TD> upper critical dimension<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | phase transition | spin glasses | external magnetic field | critical behavior | four-dimensional spin glass | glass transition | upper critical dimension | structural glasses | time-reversal symmetry | thermodynamic glass transition | janus special-purpose\"", "nodeType": "group", "penwidth": "4", "pos": "11250,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "16" }, { "_gvid": 416, "name": "group2010201221", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 84 | 96 | 225 | 249 | 257 | 263 | 267 | 318 | 367 | 375 | 376 | 394 | 406\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group2010201221", "height": "12.5", "label": "
JANUS ARCHITECTURE | SPIN GLASSES ( 2010 , 2012 ) (((2010,2012),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
janus architecture<\/TD> spin glasses<\/TD> scaling<\/TD> large systems<\/TD><\/TR>\n
cycles<\/TD> off-equilibrium dynamics<\/TD> equilibrium<\/TD> low temperature<\/TD><\/TR>\n
monte carlo simulations<\/TD> janus<\/TD> spin-glass simulation<\/TD> theoretical models<\/TD><\/TR>\n
parallel tempering<\/TD> equilibrium simulations<\/TD> gpus<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | monte carlo simulations | equilibrium | off-equilibrium dynamics | large systems | cycles | low temperature | equilibrium simulations | parallel tempering | janus | theoretical models | janus architecture | gpus | spin-glass simulation\"", "nodeType": "group", "penwidth": "4", "pos": "5306.5,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "12.5" }, { "_gvid": 417, "name": "group2010201222", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 68 | 132 | 394\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "2010", "gid": "group2010201222", "height": "7.9583", "label": "
SCALING | GPUS ( 2010 , 2012 ) (((2010,2012),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling<\/TD> gpus<\/TD> spin systems<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin systems | spin-glass model | gpus\"", "nodeType": "group", "penwidth": "4", "pos": "16106,11876", "role": "\"3.0 | 1.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "7.9583" }, { "_gvid": 418, "name": "group2010201223", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 112 | 167 | 214 | 387 | 389 | 393 | 400 | 401 | 402 | 403\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group2010201223", "height": "12.486", "label": "
SCALING RELATIONS | JAMMED PACKINGS ( 2010 , 2012 ) (((2010,2012),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling relations<\/TD> pair correlation<\/TD> jammed packings<\/TD> universal microstructure<\/TD><\/TR>\n
emergence<\/TD> granular materials<\/TD> scaling<\/TD> universal<\/TD><\/TR>\n
local structure<\/TD> spatial dimensions<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | universal | spatial dimensions | emergence | jamming | granular materials | local structure | universal microstructure | jammed packings | pair correlation | scaling relations\"", "nodeType": "group", "penwidth": "4", "pos": "17262,11876", "role": "\"3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0 | 1.0 | 2.0 | 0.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "12.486" }, { "_gvid": 419, "name": "group2010201224", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 23 | 30 | 37 | 72 | 100 | 101 | 117 | 215 | 216 | 223 | 268 | 398 | 399\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2010", "gid": "group2010201224", "height": "12.875", "label": "
GINZBURG CRITERION | SOFT MODES ( 2010 , 2012 ) (((2010,2012),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ginzburg criterion<\/TD> soft modes<\/TD> hypernetted chain approximation<\/TD> gibbs free<\/TD><\/TR>\n
dynamical transition<\/TD> critical exponents<\/TD> energy<\/TD> correlation length<\/TD><\/TR>\n
critical behavior<\/TD> correlation functions<\/TD> replicas<\/TD> field theories<\/TD><\/TR>\n
glass transition<\/TD> fluctuations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | correlation functions | field theories | energy | correlation length | fluctuations | critical behavior | replicas | dynamical transition | glass transition | gibbs free | hypernetted chain approximation | soft modes | ginzburg criterion\"", "nodeType": "group", "penwidth": "4", "pos": "15138,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "12.875" }, { "_gvid": 420, "name": "group2010201225", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 54 | 101 | 215 | 219 | 272 | 287\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group2010201225", "height": "13.347", "label": "
EQUILIBRIUM DYNAMICS | DYNAMICAL TRANSITION ( 2010 , 2012 ) (((2010,2012),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
equilibrium dynamics<\/TD> dynamical transition<\/TD> critical behavior<\/TD> critical exponents<\/TD><\/TR>\n
spin glasses<\/TD> random energy model<\/TD> mode coupling theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | spin glasses | critical behavior | dynamical transition | equilibrium dynamics | random energy model | mode coupling theory\"", "nodeType": "group", "penwidth": "4", "pos": "4303.5,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "13.347" }, { "_gvid": 421, "name": "group2010201226", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"13 | 107 | 116 | 117 | 133 | 216 | 269 | 387 | 404 | 405\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group2010201226", "height": "13.736", "label": "
DENSE AMORPHOUS HARD SPHERES | EXACT THEORY ( 2010 , 2012 ) (((2010,2012),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dense amorphous hard spheres<\/TD> exact theory<\/TD> jamming<\/TD> free energy<\/TD><\/TR>\n
replicas<\/TD> probability distribution<\/TD> hard spheres<\/TD> replica symmetry breaking<\/TD><\/TR>\n
glass transition<\/TD> structure function<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"structure function | free energy | probability distribution | replicas | replica symmetry breaking | glass transition | hard spheres | jamming | exact theory | dense amorphous hard spheres\"", "nodeType": "group", "penwidth": "4", "pos": "19724,11876", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "13.736" }, { "_gvid": 422, "name": "group2010201227", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 30 | 63 | 229 | 255 | 287\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group2010201227", "height": "11.472", "label": "
DYNAMICAL APPROACH | MEAN-FIELD MODEL ( 2010 , 2012 ) (((2010,2012),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical approach<\/TD> mean-field model<\/TD> field theories<\/TD> expansion<\/TD><\/TR>\n
p-spin model<\/TD> mode coupling theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | field theories | mean-field model | dynamical approach | p-spin model | mode coupling theory\"", "nodeType": "group", "penwidth": "4", "pos": "1687.5,11876", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "11.472" }, { "_gvid": 423, "name": "group2010201228", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 37 | 132 | 184 | 223 | 253 | 255 | 278 | 287 | 326 | 352 | 407\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2010", "gid": "group2010201228", "height": "13.472", "label": "
DYNAMICAL BEHAVIOR | ANALYTICAL PREDICTIONS ( 2010 , 2012 ) (((2010,2012),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical behavior<\/TD> analytical predictions<\/TD> gibbs free<\/TD> power law<\/TD><\/TR>\n
energy<\/TD> correlation functions<\/TD> criticality<\/TD> discontinuous transitions<\/TD><\/TR>\n
glass-forming liquids<\/TD> p-spin model<\/TD> spin-glass model<\/TD> mode coupling theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | energy | spin-glass model | power law | gibbs free | analytical predictions | p-spin model | dynamical behavior | mode coupling theory | glass-forming liquids | discontinuous transitions | criticality\"", "nodeType": "group", "penwidth": "4", "pos": "6313.5,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "13.472" }, { "_gvid": 424, "name": "group2010201229", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"30 | 62 | 75 | 112 | 133 | 136 | 242 | 307 | 407\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "2010", "gid": "group2010201229", "height": "12.125", "label": "
REPLICA EQUIVALENCE | CRITICALITY ( 2010 , 2012 ) (((2010,2012),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica equivalence<\/TD> criticality<\/TD> field theories<\/TD> replica symmetry<\/TD><\/TR>\n
order parameter<\/TD> ising spin-glasses<\/TD> replica symmetry breaking<\/TD> universal<\/TD><\/TR>\n
upper critical dimension<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"field theories | order parameter | replica symmetry | universal | replica symmetry breaking | ising spin-glasses | upper critical dimension | replica equivalence | criticality\"", "nodeType": "group", "penwidth": "4", "pos": "14018,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "12.125" }, { "_gvid": 425, "name": "group20102012210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 84 | 138 | 181 | 367 | 406\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2010", "gid": "group20102012210", "height": "11.819", "label": "
MONTE CARLO SIMULATIONS | SPIN GLASSES ( 2010 , 2012 ) (((2010,2012),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
monte carlo simulations<\/TD> spin glasses<\/TD> spin-glass simulation<\/TD> janus<\/TD><\/TR>\n
glassy systems<\/TD> statistical mechanics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | monte carlo simulations | statistical mechanics | glassy systems | janus | spin-glass simulation\"", "nodeType": "group", "penwidth": "4", "pos": "602.5,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "11.819" }, { "_gvid": 426, "name": "group20102012211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"55 | 143 | 184 | 202 | 255 | 258 | 287\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group20102012211", "height": "13.208", "label": "
SHERRINGTON-KIRKPATRICK MODEL | POWER LAW ( 2010 , 2012 ) (((2010,2012),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
sherrington-kirkpatrick model<\/TD> power law<\/TD> physical meaning<\/TD> quenched disorder<\/TD><\/TR>\n
p-spin model<\/TD> structural glasses<\/TD> mode coupling theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"sherrington-kirkpatrick model | physical meaning | power law | quenched disorder | p-spin model | structural glasses | mode coupling theory\"", "nodeType": "group", "penwidth": "4", "pos": "7492.5,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "13.208" }, { "_gvid": 427, "name": "group20102012212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"62 | 63 | 64 | 73 | 91 | 167 | 216 | 287\"", "frequence": "\"0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2010", "gid": "group20102012212", "height": "13", "label": "
FIRST-ORDER TRANSITIONS | REPLICA APPROACH ( 2010 , 2012 ) (((2010,2012),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
first-order transitions<\/TD> replica approach<\/TD> spatial dimensions<\/TD> transition<\/TD><\/TR>\n
mean-field model<\/TD> order parameter<\/TD> glass transition<\/TD> mode coupling theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"order parameter | mean-field model | replica approach | transition | first-order transitions | spatial dimensions | glass transition | mode coupling theory\"", "nodeType": "group", "penwidth": "4", "pos": "18398,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "13" }, { "_gvid": 428, "name": "group20102012213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 70 | 100 | 116 | 200\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group20102012213", "height": "12.681", "label": "
MEAN-FIELD SPIN GLASSES | MEAN-FIELD MODEL ( 2010 , 2012 ) (((2010,2012),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mean-field spin glasses<\/TD> mean-field model<\/TD> probability distribution<\/TD> magnetic field<\/TD><\/TR>\n
fluctuations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | magnetic field | fluctuations | probability distribution | mean-field spin glasses\"", "nodeType": "group", "penwidth": "4", "pos": "10146,11876", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "12.681" }, { "_gvid": 429, "name": "group20102012214", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"109 | 124 | 129 | 232 | 260 | 369 | 372\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group20102012214", "height": "10.583", "label": "
EXACT EXPRESSION | PURE STATES ( 2010 , 2012 ) (((2010,2012),2),14)<\/TD><\/TR>\n
<\/TD><\/TR>\n
exact expression<\/TD> pure states<\/TD> phase space<\/TD> matrix models<\/TD><\/TR>\n
quantum system<\/TD> partition function<\/TD> purity<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"partition function | quantum system | pure states | matrix models | phase space | purity | exact expression\"", "nodeType": "group", "penwidth": "4", "pos": "23898,11876", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "10.583" }, { "_gvid": 430, "name": "group20102012215", "bId": "5", "branchId": "0 71 1 12", "fontname": "Arial", "foundation": "\"127 | 218 | 359 | 360 | 363 | 368 | 382 | 408 | 409\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2010", "gid": "group20102012215", "height": "12.722", "label": "
NEIGHBOURS | SELF-PROPELLED PARTICLES ( 2010 , 2012 ) (((2010,2012),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
neighbours<\/TD> self-propelled particles<\/TD> topological interactions<\/TD> starling flocks<\/TD><\/TR>\n
collective animal behaviour<\/TD> bird flocks<\/TD> topology<\/TD> flocks<\/TD><\/TR>\n
external perturbation<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"topology | external perturbation | flocks | collective animal behaviour | starling flocks | topological interactions | bird flocks | self-propelled particles | neighbours\"", "nodeType": "group", "penwidth": "4", "pos": "30736,11876", "role": "\"3.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2012-10-09\"", "strTo": "\"2012-10-09\"", "support": "1", "to": "2012", "weight": "Just 1.0", "width": "12.722" }, { "_gvid": 431, "name": "period20112013", "fontsize": "50", "from": "2011", "height": "0.875", "label": "2011 2013", "nodeType": "period", "pos": "33302,10668", "shape": "box", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "to": "2013", "width": "3.9444" }, { "_gvid": 432, "name": "group2011201320", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 100 | 108 | 167 | 192 | 242 | 249\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2011", "gid": "group2011201320", "height": "12.097", "label": "
SURFACE GROWTH | LATTICE SPACING ( 2011 , 2013 ) (((2011,2013),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
surface growth<\/TD> lattice spacing<\/TD> scaling<\/TD> large systems<\/TD><\/TR>\n
fluctuations<\/TD> critical exponents<\/TD> spatial dimensions<\/TD> upper critical dimension<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | fluctuations | lattice spacing | spatial dimensions | surface growth | upper critical dimension | large systems\"", "nodeType": "group", "penwidth": "4", "pos": "18608,10668", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "12.097" }, { "_gvid": 433, "name": "group2011201321", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 11 | 30 | 67 | 92 | 97 | 117 | 188 | 216 | 255 | 410\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group2011201321", "height": "13.556", "label": "
CRITICAL PROPERTIES | SPARSE RANDOM GRAPHS ( 2011 , 2013 ) (((2011,2013),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical properties<\/TD> sparse random graphs<\/TD> field theories<\/TD> random-field ising model<\/TD><\/TR>\n
scaling<\/TD> critical points<\/TD> phase transition<\/TD> ising model<\/TD><\/TR>\n
replicas<\/TD> p-spin model<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | phase transition | field theories | critical points | critical properties | ising model | replicas | random-field ising model | glass transition | p-spin model | sparse random graphs\"", "nodeType": "group", "penwidth": "4", "pos": "22106,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "13.556" }, { "_gvid": 434, "name": "group2011201322", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 11 | 36 | 37 | 54 | 59 | 73 | 97 | 101 | 113 | 135 | 184 | 188 | 264\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group2011201322", "height": "14.486", "label": "
LONG-RANGE INTERACTIONS | LOWER CRITICAL DIMENSION ( 2011 , 2013 ) (((2011,2013),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
long-range interactions<\/TD> lower critical dimension<\/TD> scaling<\/TD> phase transition<\/TD><\/TR>\n
ising model<\/TD> zero temperature<\/TD> ground state<\/TD> random field<\/TD><\/TR>\n
spin glasses<\/TD> energy<\/TD> random-field ising model<\/TD> power law<\/TD><\/TR>\n
critical behavior<\/TD> transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | phase transition | ground state | energy | spin glasses | zero temperature | transition | ising model | critical behavior | random field | lower critical dimension | power law | random-field ising model | long-range interactions\"", "nodeType": "group", "penwidth": "4", "pos": "10782,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "14.486" }, { "_gvid": 435, "name": "group2011201323", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 27 | 76 | 101 | 112 | 136 | 285 | 304 | 367 | 403\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2011", "gid": "group2011201323", "height": "13.917", "label": "
THREE-DIMENSIONAL ISING SPIN GLASS | SCALING ( 2011 , 2013 ) (((2011,2013),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
three-dimensional ising spin glass<\/TD> scaling<\/TD> scaling relations<\/TD> universal<\/TD><\/TR>\n
ising spin-glasses<\/TD> anomalous dimensions<\/TD> edwards-anderson model<\/TD> critical temperature<\/TD><\/TR>\n
critical behavior<\/TD> janus<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | anomalous dimensions | critical temperature | critical behavior | universal | ising spin-glasses | three-dimensional ising spin glass | edwards-anderson model | janus | scaling relations\"", "nodeType": "group", "penwidth": "4", "pos": "12024,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "13.917" }, { "_gvid": 436, "name": "group2011201324", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 37 | 76 | 96 | 181 | 193 | 219 | 223 | 225\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group2011201324", "height": "12.319", "label": "
OFF-EQUILIBRIUM DYNAMICS | EQUILIBRIUM DYNAMICS ( 2011 , 2013 ) (((2011,2013),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> equilibrium dynamics<\/TD> scaling<\/TD> equilibrium<\/TD><\/TR>\n
energy<\/TD> gibbs free<\/TD> aging<\/TD> glassy systems<\/TD><\/TR>\n
critical temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | energy | critical temperature | equilibrium | glassy systems | aging | equilibrium dynamics | gibbs free | off-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "4010.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "12.319" }, { "_gvid": 437, "name": "group2011201325", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 84 | 367 | 376 | 406\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2011", "gid": "group2011201325", "height": "10.625", "label": "
JANUS ARCHITECTURE | SPIN GLASSES ( 2011 , 2013 ) (((2011,2013),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
janus architecture<\/TD> spin glasses<\/TD> janus<\/TD> monte carlo simulations<\/TD><\/TR>\n
spin-glass simulation<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | monte carlo simulations | janus | janus architecture | spin-glass simulation\"", "nodeType": "group", "penwidth": "4", "pos": "1137.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "10.625" }, { "_gvid": 438, "name": "group2011201326", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 87 | 269 | 324 | 342 | 351 | 387 | 388 | 395 | 397 | 412\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group2011201326", "height": "11.111", "label": "
ISOSTATICITY | CRYSTALS ( 2011 , 2013 ) (((2011,2013),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
isostaticity<\/TD> crystals<\/TD> hard spheres<\/TD> jamming transition<\/TD><\/TR>\n
jamming point<\/TD> packings<\/TD> spin-glass phase<\/TD> translational invariance<\/TD><\/TR>\n
scaling<\/TD> microscopic properties<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin-glass phase | hard spheres | translational invariance | packings | jamming transition | jamming | crystals | microscopic properties | jamming point | isostaticity\"", "nodeType": "group", "penwidth": "4", "pos": "21146,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "11.111" }, { "_gvid": 439, "name": "group2011201327", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 37 | 67 | 181 | 223 | 287 | 419\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group2011201327", "height": "11.028", "label": "
CRITICAL DYNAMICS | GIBBS FREE ( 2011 , 2013 ) (((2011,2013),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical dynamics<\/TD> gibbs free<\/TD> energy<\/TD> critical exponents<\/TD><\/TR>\n
glassy systems<\/TD> critical points<\/TD> mode coupling theory<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | energy | critical points | glassy systems | gibbs free | mode coupling theory | critical dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "6357.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "11.028" }, { "_gvid": 440, "name": "group2011201328", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 157 | 167 | 281 | 309\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0\"", "from": "2011", "gid": "group2011201328", "height": "11.819", "label": "
STOKES-EINSTEIN RELATION | GLASS FORMERS ( 2011 , 2013 ) (((2011,2013),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
stokes-einstein relation<\/TD> glass formers<\/TD> critical exponents<\/TD> open problems<\/TD><\/TR>\n
spatial dimensions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | open problems | spatial dimensions | glass formers | stokes-einstein relation\"", "nodeType": "group", "penwidth": "4", "pos": "17676,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "11.819" }, { "_gvid": 441, "name": "group2011201329", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 124 | 129 | 303 | 353 | 386 | 417 | 418\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group2011201329", "height": "13.792", "label": "
ENTANGLEMENT SPECTRUM | VON NEUMANN ENTROPY ( 2011 , 2013 ) (((2011,2013),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
entanglement spectrum<\/TD> von neumann entropy<\/TD> density matrix<\/TD> bipartite entanglement<\/TD><\/TR>\n
continuous phase transition<\/TD> pure states<\/TD> quantum system<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | quantum system | pure states | continuous phase transition | bipartite entanglement | density matrix | von neumann entropy | entanglement spectrum\"", "nodeType": "group", "penwidth": "4", "pos": "23310,10668", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "13.792" }, { "_gvid": 442, "name": "group20112013210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 30 | 64 | 72 | 100 | 117 | 181 | 216 | 268 | 398 | 399 | 407\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2011", "gid": "group20112013210", "height": "15.056", "label": "
GINZBURG CRITERION | HYPERNETTED CHAIN APPROXIMATION ( 2011 , 2013 ) (((2011,2013),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ginzburg criterion<\/TD> hypernetted chain approximation<\/TD> soft modes<\/TD> field theories<\/TD><\/TR>\n
correlation functions<\/TD> replicas<\/TD> correlation length<\/TD> glass transition<\/TD><\/TR>\n
fluctuations<\/TD> criticality<\/TD> glassy systems<\/TD> replica approach<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | field theories | replica approach | correlation length | fluctuations | replicas | glassy systems | glass transition | hypernetted chain approximation | soft modes | ginzburg criterion | criticality\"", "nodeType": "group", "penwidth": "4", "pos": "15006,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "15.056" }, { "_gvid": 443, "name": "group20112013211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 30 | 67 | 96 | 113 | 117 | 134 | 181 | 188 | 216 | 248 | 398\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group20112013211", "height": "11.236", "label": "
UNIVERSALITY CLASS | SOFT MODES ( 2011 , 2013 ) (((2011,2013),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
universality class<\/TD> soft modes<\/TD> field theories<\/TD> replicas<\/TD><\/TR>\n
correlation functions<\/TD> random-field ising model<\/TD> critical points<\/TD> random field<\/TD><\/TR>\n
glass transition<\/TD> glassy systems<\/TD> disorder<\/TD> equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | field theories | critical points | equilibrium | random field | replicas | disorder | glassy systems | random-field ising model | glass transition | universality class | soft modes\"", "nodeType": "group", "penwidth": "4", "pos": "13986,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "11.236" }, { "_gvid": 444, "name": "group20112013213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"39 | 59 | 64 | 68 | 75 | 77 | 107 | 154 | 188 | 189 | 315 | 410\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2011", "gid": "group20112013213", "height": "13.444", "label": "
FINITE-SIZE CORRECTIONS | RANDOM GRAPH ( 2011 , 2013 ) (((2011,2013),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-size corrections<\/TD> random graph<\/TD> sparse random graphs<\/TD> replica symmetry<\/TD><\/TR>\n
zero temperature<\/TD> cavity method<\/TD> ground-state energy<\/TD> spin systems<\/TD><\/TR>\n
free energy<\/TD> disordered systems<\/TD> replica approach<\/TD> random-field ising model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"ground-state energy | zero temperature | replica approach | spin systems | replica symmetry | disordered systems | free energy | random graph | random-field ising model | finite-size corrections | cavity method | sparse random graphs\"", "nodeType": "group", "penwidth": "4", "pos": "24916,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "13.444" }, { "_gvid": 445, "name": "group20112013214", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"48 | 54 | 77 | 84 | 134 | 202 | 414\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group20112013214", "height": "12.708", "label": "
HIERARCHICAL MODEL | SPIN GLASSES ( 2011 , 2013 ) (((2011,2013),2),14)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hierarchical model<\/TD> spin glasses<\/TD> renormalization group<\/TD> disordered systems<\/TD><\/TR>\n
disorder<\/TD> monte carlo simulations<\/TD> quenched disorder<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization group | spin glasses | disordered systems | monte carlo simulations | disorder | quenched disorder | hierarchical model\"", "nodeType": "group", "penwidth": "4", "pos": "7576.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "12.708" }, { "_gvid": 446, "name": "group20112013215", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"48 | 73 | 114 | 134 | 279 | 300 | 413 | 414 | 415 | 416\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group20112013215", "height": "12.819", "label": "
ANDERSON TRANSITION | CRITICAL DISORDER ( 2011 , 2013 ) (((2011,2013),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
anderson transition<\/TD> critical disorder<\/TD> hierarchical anderson model<\/TD> localization<\/TD><\/TR>\n
finite-dimensional systems<\/TD> infinite volume limit<\/TD> renormalization group<\/TD> disorder<\/TD><\/TR>\n
transition<\/TD> hierarchical model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization group | transition | infinite volume limit | disorder | finite-dimensional systems | localization | hierarchical anderson model | hierarchical model | critical disorder | anderson transition\"", "nodeType": "group", "penwidth": "4", "pos": "5426.5,10668", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 1.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "12.819" }, { "_gvid": 447, "name": "group20112013216", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 263 | 319 | 367\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2011", "gid": "group20112013216", "height": "10.653", "label": "
SPIN GLASSES | TEMPERATURE CHAOS ( 2011 , 2013 ) (((2011,2013),2),16)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> temperature chaos<\/TD> low temperature<\/TD> janus<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | low temperature | temperature chaos | janus\"", "nodeType": "group", "penwidth": "4", "pos": "12980,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "10.653" }, { "_gvid": 448, "name": "group20112013217", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 265 | 367 | 375 | 406\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2011", "gid": "group20112013217", "height": "9.4861", "label": "
SPIN GLASSES | JANUS ( 2011 , 2013 ) (((2011,2013),2),17)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin glasses<\/TD> janus<\/TD> theoretical models<\/TD> spin-glass simulation<\/TD><\/TR>\n
statistical physics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | statistical physics | janus | theoretical models | spin-glass simulation\"", "nodeType": "group", "penwidth": "4", "pos": "341.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "9.4861" }, { "_gvid": 449, "name": "group20112013218", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"60 | 73 | 87 | 107 | 243 | 263 | 269 | 372 | 387 | 404 | 405 | 411\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group20112013218", "height": "15.556", "label": "
GARDNER TRANSITION | DENSE AMORPHOUS HARD SPHERES ( 2011 , 2013 ) (((2011,2013),2),18)<\/TD><\/TR>\n
<\/TD><\/TR>\n
gardner transition<\/TD> dense amorphous hard spheres<\/TD> exact theory<\/TD> thermodynamic transition<\/TD><\/TR>\n
free energy<\/TD> jamming<\/TD> spin-glass phase<\/TD> hard spheres<\/TD><\/TR>\n
exact expression<\/TD> transition<\/TD> entropy<\/TD> low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"entropy | transition | spin-glass phase | free energy | thermodynamic transition | low temperature | hard spheres | exact expression | jamming | exact theory | dense amorphous hard spheres | gardner transition\"", "nodeType": "group", "penwidth": "4", "pos": "20114,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "15.556" }, { "_gvid": 450, "name": "group20112013219", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"68 | 73 | 82 | 132 | 202 | 216 | 258 | 263 | 324 | 370\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2\"", "from": "2011", "gid": "group20112013219", "height": "13.514", "label": "
SPIN-GLASS TRANSITION | TRANSLATIONAL INVARIANCE ( 2011 , 2013 ) (((2011,2013),2),19)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass transition<\/TD> translational invariance<\/TD> spin models<\/TD> transition<\/TD><\/TR>\n
spin systems<\/TD> structural glasses<\/TD> low temperature<\/TD> spin-glass model<\/TD><\/TR>\n
quenched disorder<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin systems | transition | spin models | spin-glass model | quenched disorder | glass transition | structural glasses | low temperature | translational invariance | spin-glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "16106,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "13.514" }, { "_gvid": 451, "name": "group20112013220", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"96 | 181 | 200 | 213 | 215 | 396\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group20112013220", "height": "12.125", "label": "
SLOW DYNAMICS | MEAN-FIELD SPIN GLASSES ( 2011 , 2013 ) (((2011,2013),2),20)<\/TD><\/TR>\n
<\/TD><\/TR>\n
slow dynamics<\/TD> mean-field spin glasses<\/TD> equilibrium<\/TD> glassy systems<\/TD><\/TR>\n
quasi-equilibrium<\/TD> dynamical transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"equilibrium | glassy systems | mean-field spin glasses | slow dynamics | dynamical transition | quasi-equilibrium\"", "nodeType": "group", "penwidth": "4", "pos": "2175.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "12.125" }, { "_gvid": 452, "name": "group20112013221", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"100 | 112 | 215 | 352\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "2011", "gid": "group20112013221", "height": "11.25", "label": "
DYNAMICAL TRANSITION | FLUCTUATIONS ( 2011 , 2013 ) (((2011,2013),2),21)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamical transition<\/TD> fluctuations<\/TD> discontinuous transitions<\/TD> universal<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"fluctuations | universal | dynamical transition | discontinuous transitions\"", "nodeType": "group", "penwidth": "4", "pos": "3089.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "11.25" }, { "_gvid": 453, "name": "group20112013222", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"181 | 193 | 260 | 270 | 301\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2011", "gid": "group20112013222", "height": "10.833", "label": "
FLUCTUATION DISSIPATION RELATIONS | AGING ( 2011 , 2013 ) (((2011,2013),2),22)<\/TD><\/TR>\n
<\/TD><\/TR>\n
fluctuation dissipation relations<\/TD> aging<\/TD> glassy systems<\/TD> phase space<\/TD><\/TR>\n
supercooled liquid<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"glassy systems | aging | phase space | fluctuation dissipation relations | supercooled liquid\"", "nodeType": "group", "penwidth": "4", "pos": "8496.5,10668", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2013-10-09\"", "strTo": "\"2013-10-09\"", "support": "1", "to": "2013", "weight": "Just 1.0", "width": "10.833" }, { "_gvid": 454, "name": "period20122014", "fontsize": "50", "from": "2012", "height": "0.875", "label": "2012 2014", "nodeType": "period", "pos": "33302,9446", "shape": "box", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "to": "2014", "width": "3.9444" }, { "_gvid": 455, "name": "group2012201420", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 113 | 134 | 204 | 414\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group2012201420", "height": "10.361", "label": "
DISORDERED MODEL | RANDOM FIELD ( 2012 , 2014 ) (((2012,2014),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
disordered model<\/TD> random field<\/TD> disorder<\/TD> hierarchical model<\/TD><\/TR>\n
critical exponents<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | random field | disorder | disordered model | hierarchical model\"", "nodeType": "group", "penwidth": "4", "pos": "21100,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "10.361" }, { "_gvid": 456, "name": "group2012201421", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 8 | 11 | 54 | 69 | 96 | 100 | 126 | 285 | 340 | 346 | 367\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2012", "gid": "group2012201421", "height": "16.389", "label": "
EQUILIBRIUM BEHAVIOUR | PROBABILITY DISTRIBUTION FUNCTION ( 2012 , 2014 ) (((2012,2014),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
equilibrium behaviour<\/TD> probability distribution function<\/TD> thermodynamical limit<\/TD> scaling<\/TD><\/TR>\n
external magnetic field<\/TD> spin glasses<\/TD> three-dimensional ising spin glass<\/TD> phase transition<\/TD><\/TR>\n
scale invariance<\/TD> equilibrium<\/TD> fluctuations<\/TD> janus<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | scale invariance | phase transition | spin glasses | external magnetic field | equilibrium | fluctuations | thermodynamical limit | three-dimensional ising spin glass | probability distribution function | equilibrium behaviour | janus\"", "nodeType": "group", "penwidth": "4", "pos": "13856,9446", "role": "\"3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "16.389" }, { "_gvid": 457, "name": "group2012201422", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 68 | 84 | 367 | 375\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2012", "gid": "group2012201422", "height": "9.3611", "label": "
THEORETICAL MODELS | SPIN GLASSES ( 2012 , 2014 ) (((2012,2014),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
theoretical models<\/TD> spin glasses<\/TD> janus<\/TD> scaling<\/TD><\/TR>\n
monte carlo simulations<\/TD> spin systems<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | spin systems | monte carlo simulations | janus | theoretical models\"", "nodeType": "group", "penwidth": "4", "pos": "1137.5,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "9.3611" }, { "_gvid": 458, "name": "group2012201423", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 77 | 96 | 137 | 138 | 258 | 422\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group2012201423", "height": "11.736", "label": "
ERGODICITY BREAKING | THERMODYNAMICS ( 2012 , 2014 ) (((2012,2014),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ergodicity breaking<\/TD> thermodynamics<\/TD> scaling<\/TD> equilibrium<\/TD><\/TR>\n
statistical mechanics<\/TD> disordered systems<\/TD> structural glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | disordered systems | equilibrium | thermodynamics | statistical mechanics | structural glasses | ergodicity breaking\"", "nodeType": "group", "penwidth": "4", "pos": "16004,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "11.736" }, { "_gvid": 459, "name": "group2012201425", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 11 | 48 | 77 | 113 | 414\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group2012201425", "height": "12.889", "label": "
HIERARCHICAL MODEL | RENORMALIZATION GROUP ( 2012 , 2014 ) (((2012,2014),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hierarchical model<\/TD> renormalization group<\/TD> random field<\/TD> disordered systems<\/TD><\/TR>\n
critical exponents<\/TD> phase transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | phase transition | renormalization group | disordered systems | random field | hierarchical model\"", "nodeType": "group", "penwidth": "4", "pos": "7582.5,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "12.889" }, { "_gvid": 460, "name": "group2012201426", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 23 | 48 | 97 | 101 | 141 | 184\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group2012201426", "height": "12.375", "label": "
FINITE-SIZE EFFECT | CORRELATION FUNCTIONS ( 2012 , 2014 ) (((2012,2014),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-size effect<\/TD> correlation functions<\/TD> critical behavior<\/TD> power law<\/TD><\/TR>\n
critical exponents<\/TD> ising model<\/TD> renormalization group<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | correlation functions | renormalization group | ising model | critical behavior | finite-size effect | power law\"", "nodeType": "group", "penwidth": "4", "pos": "8727.5,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "12.375" }, { "_gvid": 461, "name": "group2012201427", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 54 | 63 | 117 | 132 | 133 | 258 | 269 | 286 | 351 | 401 | 404 | 405 | 411\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group2012201427", "height": "15.639", "label": "
FULL REPLICA SYMMETRY BREAKING | GARDNER TRANSITION ( 2012 , 2014 ) (((2012,2014),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
full replica symmetry breaking<\/TD> gardner transition<\/TD> hard spheres<\/TD> dense amorphous hard spheres<\/TD><\/TR>\n
exact theory<\/TD> jammed packings<\/TD> replica symmetry breaking<\/TD> jamming transition<\/TD><\/TR>\n
replicas<\/TD> structural glasses<\/TD> critical exponents<\/TD> spin-glass model<\/TD><\/TR>\n
spin glasses<\/TD> mean-field model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | spin glasses | mean-field model | replicas | spin-glass model | replica symmetry breaking | structural glasses | hard spheres | full replica symmetry breaking | jamming transition | jammed packings | exact theory | dense amorphous hard spheres | gardner transition\"", "nodeType": "group", "penwidth": "4", "pos": "18972,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "15.639" }, { "_gvid": 462, "name": "group2012201428", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 107 | 127 | 186 | 258 | 334 | 351 | 387 | 389 | 409 | 412 | 421\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group2012201428", "height": "12.528", "label": "
MARGINAL STABILITY | AMORPHOUS SOLIDS ( 2012 , 2014 ) (((2012,2014),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
marginal stability<\/TD> amorphous solids<\/TD> free-energy landscape<\/TD> isostaticity<\/TD><\/TR>\n
topology<\/TD> neighbours<\/TD> granular materials<\/TD> critical exponents<\/TD><\/TR>\n
free energy<\/TD> jamming transition<\/TD> jamming<\/TD> structural glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | free energy | topology | free-energy landscape | structural glasses | amorphous solids | jamming transition | jamming | granular materials | neighbours | isostaticity | marginal stability\"", "nodeType": "group", "penwidth": "4", "pos": "20204,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "12.528" }, { "_gvid": 463, "name": "group2012201429", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 23 | 59 | 67 | 188 | 317 | 350\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "2012", "gid": "group2012201429", "height": "13.319", "label": "
LARGE DEVIATIONS | RANDOM-FIELD ISING MODEL ( 2012 , 2014 ) (((2012,2014),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
large deviations<\/TD> random-field ising model<\/TD> bethe lattice<\/TD> phase transition<\/TD><\/TR>\n
critical points<\/TD> zero temperature<\/TD> correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | correlation functions | zero temperature | critical points | random-field ising model | bethe lattice | large deviations\"", "nodeType": "group", "penwidth": "4", "pos": "12714,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "13.319" }, { "_gvid": 464, "name": "group20122014210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 48 | 53 | 64 | 167 | 216 | 275 | 281 | 302 | 309 | 313\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group20122014210", "height": "13.083", "label": "
DYNAMIC GLASS TRANSITION | SIMPLE GLASSES ( 2012 , 2014 ) (((2012,2014),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
dynamic glass transition<\/TD> simple glasses<\/TD> glass formers<\/TD> stokes-einstein relation<\/TD><\/TR>\n
mean field theory<\/TD> molecular dynamics<\/TD> phase transition<\/TD> spatial dimensions<\/TD><\/TR>\n
renormalization group<\/TD> replica approach<\/TD> glass transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | renormalization group | mean field theory | replica approach | spatial dimensions | glass transition | molecular dynamics | glass formers | simple glasses | stokes-einstein relation | dynamic glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "17574,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "13.083" }, { "_gvid": 465, "name": "group20122014211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 73 | 92 | 96 | 117 | 216 | 224 | 245 | 269 | 341\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group20122014211", "height": "12.417", "label": "
IDEAL GLASS TRANSITION | BINARY MIXTURES ( 2012 , 2014 ) (((2012,2014),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ideal glass transition<\/TD> binary mixtures<\/TD> configurational entropy<\/TD> phase transition<\/TD><\/TR>\n
critical properties<\/TD> glass transition<\/TD> replicas<\/TD> transition<\/TD><\/TR>\n
equilibrium<\/TD> hard spheres<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | transition | critical properties | equilibrium | replicas | glass transition | configurational entropy | binary mixtures | hard spheres | ideal glass transition\"", "nodeType": "group", "penwidth": "4", "pos": "22704,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "12.417" }, { "_gvid": 466, "name": "group20122014212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"12 | 23 | 76 | 84 | 132 | 133 | 141 | 195 | 213 | 230 | 304\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group20122014212", "height": "14.361", "label": "
LOW-TEMPERATURE PHASE | FINITE-SIZE EFFECT ( 2012 , 2014 ) (((2012,2014),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
low-temperature phase<\/TD> finite-size effect<\/TD> edwards-anderson model<\/TD> slow dynamics<\/TD><\/TR>\n
four-dimensional spin glass<\/TD> critical temperature<\/TD> correlation functions<\/TD> replica symmetry breaking<\/TD><\/TR>\n
spin-glass model<\/TD> asymptotic behaviour<\/TD> monte carlo simulations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"asymptotic behaviour | correlation functions | critical temperature | monte carlo simulations | spin-glass model | replica symmetry breaking | finite-size effect | four-dimensional spin glass | slow dynamics | low-temperature phase | edwards-anderson model\"", "nodeType": "group", "penwidth": "4", "pos": "10054,9446", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "14.361" }, { "_gvid": 467, "name": "group20122014213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"16 | 37 | 134 | 413\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2012", "gid": "group20122014213", "height": "10.569", "label": "
HIERARCHICAL ANDERSON MODEL | DISORDER ( 2012 , 2014 ) (((2012,2014),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hierarchical anderson model<\/TD> disorder<\/TD> energy<\/TD> renormalization<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization | energy | disorder | hierarchical anderson model\"", "nodeType": "group", "penwidth": "4", "pos": "5863.5,9446", "role": "\"3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "10.569" }, { "_gvid": 468, "name": "group20122014214", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"31 | 54 | 132 | 317 | 407 | 419\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0\"", "from": "2012", "gid": "group20122014214", "height": "10.264", "label": "
CRITICAL DYNAMICS | BETHE LATTICE ( 2012 , 2014 ) (((2012,2014),2),14)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical dynamics<\/TD> bethe lattice<\/TD> spin-glass model<\/TD> criticality<\/TD><\/TR>\n
spin glasses<\/TD> divergence<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"divergence | spin glasses | spin-glass model | bethe lattice | criticality | critical dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "5041.5,9446", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "10.264" }, { "_gvid": 469, "name": "group20122014215", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 69 | 70 | 215 | 225 | 258 | 263 | 285 | 370 | 380\"", "frequence": "\"5.555555555555558e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "2012", "gid": "group20122014215", "height": "12.972", "label": "
JANUS SPECIAL-PURPOSE | SPIN GLASSES ( 2012 , 2014 ) (((2012,2014),2),15)<\/TD><\/TR>\n
<\/TD><\/TR>\n
janus special-purpose<\/TD> spin glasses<\/TD> spin-glass transition<\/TD> external magnetic field<\/TD><\/TR>\n
three-dimensional ising spin glass<\/TD> low temperature<\/TD> structural glasses<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
magnetic field<\/TD> dynamical transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | external magnetic field | magnetic field | dynamical transition | off-equilibrium dynamics | structural glasses | low temperature | three-dimensional ising spin glass | spin-glass transition | janus special-purpose\"", "nodeType": "group", "penwidth": "4", "pos": "11110,9446", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "12.972" }, { "_gvid": 470, "name": "group20122014217", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"81 | 100 | 154 | 189 | 237\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2012", "gid": "group20122014217", "height": "11.403", "label": "
ANALYTICAL SOLUTION | RANDOM GRAPH ( 2012 , 2014 ) (((2012,2014),2),17)<\/TD><\/TR>\n
<\/TD><\/TR>\n
analytical solution<\/TD> random graph<\/TD> finite-size corrections<\/TD> fluctuations<\/TD><\/TR>\n
excellent agreement<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"excellent agreement | fluctuations | random graph | finite-size corrections | analytical solution\"", "nodeType": "group", "penwidth": "4", "pos": "24916,9446", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2014-10-09\"", "strTo": "\"2014-10-09\"", "support": "1", "to": "2014", "weight": "Just 1.0", "width": "11.403" }, { "_gvid": 471, "name": "period20132015", "fontsize": "50", "from": "2013", "height": "0.875", "label": "2013 2015", "nodeType": "period", "pos": "33302,8265", "shape": "box", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "to": "2015", "width": "3.9444" }, { "_gvid": 472, "name": "group2013201520", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 100 | 167 | 192 | 248\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2013", "gid": "group2013201520", "height": "11.083", "label": "
SURFACE GROWTH | SPATIAL DIMENSIONS ( 2013 , 2015 ) (((2013,2015),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
surface growth<\/TD> spatial dimensions<\/TD> critical exponents<\/TD> scaling<\/TD><\/TR>\n
fluctuations<\/TD> universality class<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | fluctuations | spatial dimensions | surface growth | universality class\"", "nodeType": "group", "penwidth": "4", "pos": "17946,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "11.083" }, { "_gvid": 473, "name": "group2013201521", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 112 | 167 | 184 | 331 | 342 | 351 | 387 | 401 | 403 | 407\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2013", "gid": "group2013201521", "height": "10.903", "label": "
INFINITE DIMENSIONS | SCALING ( 2013 , 2015 ) (((2013,2015),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
infinite dimensions<\/TD> scaling<\/TD> scaling relations<\/TD> jammed packings<\/TD><\/TR>\n
critical exponents<\/TD> packings<\/TD> universal<\/TD> power law<\/TD><\/TR>\n
jamming transition<\/TD> spatial dimensions<\/TD> jamming<\/TD> criticality<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | universal | spatial dimensions | power law | infinite dimensions | packings | jamming transition | jamming | jammed packings | scaling relations | criticality\"", "nodeType": "group", "penwidth": "4", "pos": "19296,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "10.903" }, { "_gvid": 474, "name": "group2013201522", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 11 | 31 | 53 | 54 | 61 | 72 | 76 | 132 | 135 | 210\"", "frequence": "\"0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0\"", "from": "2013", "gid": "group2013201522", "height": "14.389", "label": "
FINITE-SIZE SCALING TECHNIQUES | LOWER CRITICAL DIMENSION ( 2013 , 2015 ) (((2013,2015),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-size scaling techniques<\/TD> lower critical dimension<\/TD> probability<\/TD> phase transition<\/TD><\/TR>\n
correlation length<\/TD> divergence<\/TD> mean field theory<\/TD> spin glasses<\/TD><\/TR>\n
critical exponents<\/TD> critical temperature<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | phase transition | divergence | mean field theory | spin glasses | probability | correlation length | critical temperature | spin-glass model | lower critical dimension | finite-size scaling techniques\"", "nodeType": "group", "penwidth": "4", "pos": "7323.5,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "14.389" }, { "_gvid": 475, "name": "group2013201523", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 48 | 54 | 69 | 73 | 97 | 136 | 304\"", "frequence": "\"0.0 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2013", "gid": "group2013201523", "height": "13.722", "label": "
ISING SPIN-GLASSES | EXTERNAL MAGNETIC FIELD ( 2013 , 2015 ) (((2013,2015),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ising spin-glasses<\/TD> external magnetic field<\/TD> spin glasses<\/TD> edwards-anderson model<\/TD><\/TR>\n
renormalization group<\/TD> ising model<\/TD> critical exponents<\/TD> transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | renormalization group | spin glasses | external magnetic field | transition | ising model | ising spin-glasses | edwards-anderson model\"", "nodeType": "group", "penwidth": "4", "pos": "8553.5,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "13.722" }, { "_gvid": 476, "name": "group2013201526", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"18 | 68 | 96 | 181 | 258 | 260 | 268\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group2013201526", "height": "11.972", "label": "
HYPERNETTED CHAIN APPROXIMATION | PHASE SPACE ( 2013 , 2015 ) (((2013,2015),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hypernetted chain approximation<\/TD> phase space<\/TD> glassy systems<\/TD> equilibrium<\/TD><\/TR>\n
structural glasses<\/TD> spin systems<\/TD> spherical model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spherical model | spin systems | equilibrium | glassy systems | structural glasses | phase space | hypernetted chain approximation\"", "nodeType": "group", "penwidth": "4", "pos": "15464,8265", "role": "\"2.0 | 2.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "11.972" }, { "_gvid": 477, "name": "group2013201527", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 54 | 87 | 116 | 141 | 143 | 200 | 286 | 333 | 425\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group2013201527", "height": "13.403", "label": "
BRANCHING TREE | CAVITY APPROACH ( 2013 , 2015 ) (((2013,2015),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
branching tree<\/TD> cavity approach<\/TD> physical meaning<\/TD> probability distribution<\/TD><\/TR>\n
correlation functions<\/TD> spin glasses<\/TD> full replica symmetry breaking<\/TD> finite-size effect<\/TD><\/TR>\n
spin-glass phase<\/TD> mean-field spin glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | spin glasses | spin-glass phase | probability distribution | finite-size effect | physical meaning | mean-field spin glasses | full replica symmetry breaking | cavity approach | branching tree\"", "nodeType": "group", "penwidth": "4", "pos": "9602.5,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "13.403" }, { "_gvid": 478, "name": "group2013201528", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"31 | 61 | 73 | 100 | 154 | 197 | 409\"", "frequence": "\"0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group2013201528", "height": "9.1389", "label": "
BIFURCATION | DIVERGENCE ( 2013 , 2015 ) (((2013,2015),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
bifurcation<\/TD> divergence<\/TD> random graph<\/TD> probability<\/TD><\/TR>\n
fluctuations<\/TD> transition<\/TD> neighbours<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"divergence | probability | transition | fluctuations | random graph | bifurcation | neighbours\"", "nodeType": "group", "penwidth": "4", "pos": "24874,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "9.1389" }, { "_gvid": 479, "name": "group2013201529", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 54 | 113 | 300 | 398\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group2013201529", "height": "9.4722", "label": "
LOCALIZATION | RANDOM FIELD ( 2013 , 2015 ) (((2013,2015),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
localization<\/TD> random field<\/TD> soft modes<\/TD> spin glasses<\/TD><\/TR>\n
energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | spin glasses | random field | localization | soft modes\"", "nodeType": "group", "penwidth": "4", "pos": "11528,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "9.4722" }, { "_gvid": 480, "name": "group20132015210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 63 | 84 | 87 | 167 | 216 | 237 | 301 | 326\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2013", "gid": "group20132015210", "height": "13.361", "label": "
GLASS-FORMING LIQUIDS | SUPERCOOLED LIQUID ( 2013 , 2015 ) (((2013,2015),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glass-forming liquids<\/TD> supercooled liquid<\/TD> analytical solution<\/TD> mean field theory<\/TD><\/TR>\n
mean-field model<\/TD> spatial dimensions<\/TD> glass transition<\/TD> monte carlo simulations<\/TD><\/TR>\n
spin-glass phase<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | mean-field model | monte carlo simulations | spin-glass phase | spatial dimensions | glass transition | analytical solution | supercooled liquid | glass-forming liquids\"", "nodeType": "group", "penwidth": "4", "pos": "16848,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "13.361" }, { "_gvid": 481, "name": "group20132015211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 73 | 157 | 181 | 216 | 225 | 236 | 242 | 263 | 269 | 387\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group20132015211", "height": "11.75", "label": "
SOFT SPHERES | TRANSITION ( 2013 , 2015 ) (((2013,2015),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
soft spheres<\/TD> transition<\/TD> upper critical dimension<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
glass transition<\/TD> open problems<\/TD> mean-field model<\/TD> glassy systems<\/TD><\/TR>\n
hard spheres<\/TD> low temperature<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | transition | open problems | glassy systems | glass transition | off-equilibrium dynamics | soft spheres | upper critical dimension | low temperature | hard spheres | jamming\"", "nodeType": "group", "penwidth": "4", "pos": "21650,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "11.75" }, { "_gvid": 482, "name": "group20132015212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"77 | 87 | 112 | 273 | 311 | 351 | 387 | 398 | 412\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group20132015212", "height": "14.417", "label": "
VIBRATIONAL SPECTRUM | POTENTIAL ENERGY LANDSCAPE ( 2013 , 2015 ) (((2013,2015),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
vibrational spectrum<\/TD> potential energy landscape<\/TD> isostaticity<\/TD> spin-glass phase<\/TD><\/TR>\n
universal<\/TD> disordered systems<\/TD> jamming transition<\/TD> jamming<\/TD><\/TR>\n
soft modes<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"disordered systems | spin-glass phase | universal | potential energy landscape | vibrational spectrum | jamming transition | jamming | soft modes | isostaticity\"", "nodeType": "group", "penwidth": "4", "pos": "22664,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "14.417" }, { "_gvid": 483, "name": "group20132015213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"96 | 181 | 193 | 219 | 235 | 260 | 263 | 287 | 396\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group20132015213", "height": "11.875", "label": "
GLASSY SYSTEMS | HYPERNETTED CHAIN ( 2013 , 2015 ) (((2013,2015),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
glassy systems<\/TD> hypernetted chain<\/TD> equilibrium dynamics<\/TD> equilibrium<\/TD><\/TR>\n
aging<\/TD> quasi-equilibrium<\/TD> mode coupling theory<\/TD> phase space<\/TD><\/TR>\n
low temperature<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"equilibrium | glassy systems | aging | equilibrium dynamics | hypernetted chain | phase space | low temperature | mode coupling theory | quasi-equilibrium\"", "nodeType": "group", "penwidth": "4", "pos": "4010.5,8265", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "11.875" }, { "_gvid": 484, "name": "group20132015214", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"134 | 136 | 225 | 233 | 304 | 394 | 409\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2013", "gid": "group20132015214", "height": "14.361", "label": "
GPUS | THREE-DIMENSIONAL ISING SPIN GLASS MODEL ( 2013 , 2015 ) (((2013,2015),2),14)<\/TD><\/TR>\n
<\/TD><\/TR>\n
gpus<\/TD> three-dimensional ising spin glass model<\/TD> ising spin-glasses<\/TD> disorder<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> edwards-anderson model<\/TD> neighbours<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"disorder | ising spin-glasses | off-equilibrium dynamics | three-dimensional ising spin glass model | edwards-anderson model | gpus | neighbours\"", "nodeType": "group", "penwidth": "4", "pos": "5651.5,8265", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2015-10-09\"", "strTo": "\"2015-10-09\"", "support": "1", "to": "2015", "weight": "Just 1.0", "width": "14.361" }, { "_gvid": 485, "name": "period20142016", "fontsize": "50", "from": "2014", "height": "0.875", "label": "2014 2016", "nodeType": "period", "pos": "33302,7158", "shape": "box", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "to": "2016", "width": "3.9444" }, { "_gvid": 486, "name": "group2014201620", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 27 | 54 | 72 | 101 | 112 | 116 | 136 | 167\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2014", "gid": "group2014201620", "height": "13.083", "label": "
CRITICAL EXPONENTS | PROBABILITY DISTRIBUTION ( 2014 , 2016 ) (((2014,2016),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical exponents<\/TD> probability distribution<\/TD> correlation length<\/TD> scaling<\/TD><\/TR>\n
spin glasses<\/TD> anomalous dimensions<\/TD> ising spin-glasses<\/TD> critical behavior<\/TD><\/TR>\n
universal<\/TD> spatial dimensions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | anomalous dimensions | spin glasses | correlation length | critical behavior | universal | probability distribution | ising spin-glasses | spatial dimensions\"", "nodeType": "group", "penwidth": "4", "pos": "11098,7158", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "13.083" }, { "_gvid": 487, "name": "group2014201621", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 14 | 39 | 100 | 149 | 351 | 387 | 397\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2014", "gid": "group2014201621", "height": "10.111", "label": "
JAMMING POINT | SCALING ( 2014 , 2016 ) (((2014,2016),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
jamming point<\/TD> scaling<\/TD> ground-state energy<\/TD> expansion<\/TD><\/TR>\n
phase diagram<\/TD> jamming transition<\/TD> fluctuations<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | expansion | ground-state energy | fluctuations | phase diagram | jamming transition | jamming | jamming point\"", "nodeType": "group", "penwidth": "4", "pos": "19770,7158", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "10.111" }, { "_gvid": 488, "name": "group2014201622", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 63 | 103 | 112 | 167 | 236 | 279 | 334 | 342 | 344 | 351 | 387\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2014", "gid": "group2014201622", "height": "13.778", "label": "
AMORPHOUS PACKINGS | FINITE-DIMENSIONAL SYSTEMS ( 2014 , 2016 ) (((2014,2016),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
amorphous packings<\/TD> finite-dimensional systems<\/TD> packings<\/TD> scaling<\/TD><\/TR>\n
universal<\/TD> mean-field model<\/TD> spatial dimensions<\/TD> exact solution<\/TD><\/TR>\n
soft spheres<\/TD> amorphous solids<\/TD> jamming transition<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | mean-field model | exact solution | universal | spatial dimensions | soft spheres | finite-dimensional systems | amorphous solids | packings | amorphous packings | jamming transition | jamming\"", "nodeType": "group", "penwidth": "4", "pos": "20848,7158", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "13.778" }, { "_gvid": 489, "name": "group2014201623", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 54 | 73 | 76 | 96 | 101 | 225 | 233\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2014", "gid": "group2014201623", "height": "14.333", "label": "
THREE-DIMENSIONAL ISING SPIN GLASS MODEL | SPIN GLASSES ( 2014 , 2016 ) (((2014,2016),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
three-dimensional ising spin glass model<\/TD> spin glasses<\/TD> critical exponents<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
critical temperature<\/TD> critical behavior<\/TD> transition<\/TD> equilibrium<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | spin glasses | transition | critical temperature | equilibrium | critical behavior | off-equilibrium dynamics | three-dimensional ising spin glass model\"", "nodeType": "group", "penwidth": "4", "pos": "7949.5,7158", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "14.333" }, { "_gvid": 490, "name": "group2014201624", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 37 | 73 | 87 | 112 | 213 | 263 | 302 | 323 | 334\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2014", "gid": "group2014201624", "height": "10.542", "label": "
BOSON PEAK | SIMPLE GLASSES ( 2014 , 2016 ) (((2014,2016),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
boson peak<\/TD> simple glasses<\/TD> slow dynamics<\/TD> phase transition<\/TD><\/TR>\n
transition<\/TD> spin-glass phase<\/TD> universal<\/TD> low temperature<\/TD><\/TR>\n
amorphous solids<\/TD> energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | energy | transition | spin-glass phase | universal | slow dynamics | low temperature | simple glasses | boson peak | amorphous solids\"", "nodeType": "group", "penwidth": "4", "pos": "15828,7158", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "10.542" }, { "_gvid": 491, "name": "group2014201625", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 16 | 30 | 37 | 57 | 83 | 92 | 100 | 101 | 132 | 184\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0\"", "from": "2014", "gid": "group2014201625", "height": "10.722", "label": "
SPECIFIC HEAT | SPIN GLASS THEORY ( 2014 , 2016 ) (((2014,2016),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
specific heat<\/TD> spin glass theory<\/TD> renormalization<\/TD> expansion<\/TD><\/TR>\n
field theories<\/TD> energy<\/TD> critical properties<\/TD> power law<\/TD><\/TR>\n
critical behavior<\/TD> fluctuations<\/TD> spin-glass model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | renormalization | field theories | energy | specific heat | spin glass theory | critical properties | fluctuations | critical behavior | spin-glass model | power law\"", "nodeType": "group", "penwidth": "4", "pos": "4919.5,7158", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "10.722" }, { "_gvid": 492, "name": "group2014201626", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 102 | 107 | 319 | 390\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2014", "gid": "group2014201626", "height": "9.2917", "label": "
COLLOIDS | SPIN GLASSES ( 2014 , 2016 ) (((2014,2016),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
colloids<\/TD> spin glasses<\/TD> polymer<\/TD> temperature chaos<\/TD><\/TR>\n
free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | polymer | free energy | temperature chaos | colloids\"", "nodeType": "group", "penwidth": "4", "pos": "11976,7158", "role": "\"3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "9.2917" }, { "_gvid": 493, "name": "group2014201627", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 73 | 157 | 181 | 216 | 225 | 236 | 242 | 263 | 269 | 387\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2014", "gid": "group2014201627", "height": "12.681", "label": "
UPPER CRITICAL DIMENSION | SOFT SPHERES ( 2014 , 2016 ) (((2014,2016),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
upper critical dimension<\/TD> soft spheres<\/TD> mean-field model<\/TD> transition<\/TD><\/TR>\n
open problems<\/TD> glass transition<\/TD> glassy systems<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
hard spheres<\/TD> low temperature<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | transition | open problems | glassy systems | glass transition | off-equilibrium dynamics | soft spheres | upper critical dimension | low temperature | hard spheres | jamming\"", "nodeType": "group", "penwidth": "4", "pos": "23830,7158", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "12.681" }, { "_gvid": 494, "name": "group2014201628", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"133 | 145 | 262 | 265 | 269 | 387 | 412\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2014", "gid": "group2014201628", "height": "12.181", "label": "
REPLICA SYMMETRY BREAKING | NEURAL NETWORK ( 2014 , 2016 ) (((2014,2016),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica symmetry breaking<\/TD> statistical physics<\/TD> large class<\/TD> neural network<\/TD><\/TR>\n
isostaticity<\/TD> jamming<\/TD> hard spheres<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica symmetry breaking | neural network | large class | statistical physics | hard spheres | jamming | isostaticity\"", "nodeType": "group", "penwidth": "4", "pos": "18456,7158", "role": "\"3.0 | 1.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2016-10-09\"", "strTo": "\"2016-10-09\"", "support": "1", "to": "2016", "weight": "Just 1.0", "width": "12.181" }, { "_gvid": 495, "name": "period20152017", "fontsize": "50", "from": "2015", "height": "0.875", "label": "2015 2017", "nodeType": "period", "pos": "33302,6091.5", "shape": "box", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "to": "2017", "width": "3.9444" }, { "_gvid": 496, "name": "group2015201720", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 6 | 73 | 77 | 93 | 97 | 101 | 133 | 149 | 156 | 236 | 248 | 265 | 345 | 351 | 387\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2015", "gid": "group2015201720", "height": "12.139", "label": "
COMPUTER SCIENCE | COMPLEXITY ( 2015 , 2017 ) (((2015,2017),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
computer science<\/TD> complexity<\/TD> scaling<\/TD> potts model<\/TD><\/TR>\n
critical exponents<\/TD> transition<\/TD> phase diagram<\/TD> universality class<\/TD><\/TR>\n
ising model<\/TD> replica symmetry breaking<\/TD> disordered systems<\/TD> critical behavior<\/TD><\/TR>\n
statistical physics<\/TD> soft spheres<\/TD> jamming transition<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | critical exponents | transition | disordered systems | potts model | ising model | critical behavior | replica symmetry breaking | phase diagram | complexity | soft spheres | universality class | statistical physics | computer science | jamming transition | jamming\"", "nodeType": "group", "penwidth": "4", "pos": "19696,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 1.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "12.139" }, { "_gvid": 497, "name": "group2015201722", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 23 | 100 | 343 | 362 | 401\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2015", "gid": "group2015201722", "height": "12.333", "label": "
DENSITY FLUCTUATIONS | PAIR CORRELATION FUNCTION ( 2015 , 2017 ) (((2015,2017),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
density fluctuations<\/TD> pair correlation function<\/TD> scaling<\/TD> fluctuations<\/TD><\/TR>\n
correlation functions<\/TD> jammed packings<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | correlation functions | fluctuations | pair correlation function | density fluctuations | jammed packings\"", "nodeType": "group", "penwidth": "4", "pos": "16470,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "12.333" }, { "_gvid": 498, "name": "group2015201723", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 23 | 326 | 367 | 428 | 429\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2015", "gid": "group2015201723", "height": "12.361", "label": "
FREE ENERGY BARRIERS | SPIN-GLASS COHERENCE ( 2015 , 2017 ) (((2015,2017),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
free energy barriers<\/TD> spin-glass coherence<\/TD> janus<\/TD> glass-forming liquids<\/TD><\/TR>\n
correlation functions<\/TD> scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | correlation functions | glass-forming liquids | janus | spin-glass coherence | free energy barriers\"", "nodeType": "group", "penwidth": "4", "pos": "6478.5,6091.5", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "12.361" }, { "_gvid": 499, "name": "group2015201724", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 14 | 30 | 32 | 33 | 43 | 48 | 53 | 67 | 79 | 317\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2\"", "from": "2015", "gid": "group2015201724", "height": "12.792", "label": "
LOOP EXPANSION | CRITICAL POINTS ( 2015 , 2017 ) (((2015,2017),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
loop expansion<\/TD> critical points<\/TD> second order phase transition<\/TD> perturbative expansion<\/TD><\/TR>\n
field theories<\/TD> feynman diagram<\/TD> critical exponents<\/TD> renormalization group<\/TD><\/TR>\n
expansion<\/TD> mean field theory<\/TD> bethe lattice<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | expansion | field theories | perturbative expansion | second order phase transition | feynman diagram | renormalization group | mean field theory | critical points | loop expansion | bethe lattice\"", "nodeType": "group", "penwidth": "4", "pos": "13688,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "12.792" }, { "_gvid": 500, "name": "group2015201725", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 23 | 62 | 72 | 112 | 334 | 407\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2015", "gid": "group2015201725", "height": "12", "label": "
PHASE TRANSITION | AMORPHOUS SOLIDS ( 2015 , 2017 ) (((2015,2017),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
phase transition<\/TD> amorphous solids<\/TD> universal<\/TD> order parameter<\/TD><\/TR>\n
criticality<\/TD> correlation length<\/TD> correlation functions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | correlation functions | order parameter | correlation length | universal | amorphous solids | criticality\"", "nodeType": "group", "penwidth": "4", "pos": "14798,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "12" }, { "_gvid": 501, "name": "group2015201726", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"16 | 30 | 32 | 43 | 50 | 107 | 427\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "2015", "gid": "group2015201726", "height": "13.25", "label": "
TWO-LOOP CORRECTIONS | LARGE-ORDER BEHAVIOR ( 2015 , 2017 ) (((2015,2017),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
two-loop corrections<\/TD> large-order behavior<\/TD> perturbative expansion<\/TD> field theories<\/TD><\/TR>\n
feynman diagram<\/TD> renormalization<\/TD> free energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"renormalization | field theories | perturbative expansion | feynman diagram | large-order behavior | free energy | two-loop corrections\"", "nodeType": "group", "penwidth": "4", "pos": "4814.5,6091.5", "role": "\"2.0 | 3.0 | 2.0 | 1.0 | 1.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "13.25" }, { "_gvid": 502, "name": "group2015201728", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 76 | 87 | 96 | 116 | 218 | 315 | 317 | 421\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0\"", "from": "2015", "gid": "group2015201728", "height": "12.861", "label": "
MARGINAL STABILITY | EXTERNAL PERTURBATION ( 2015 , 2017 ) (((2015,2017),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
marginal stability<\/TD> cavity method<\/TD> external perturbation<\/TD> probability distribution<\/TD><\/TR>\n
spin glasses<\/TD> equilibrium<\/TD> critical temperature<\/TD> spin-glass phase<\/TD><\/TR>\n
bethe lattice<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | critical temperature | spin-glass phase | equilibrium | probability distribution | external perturbation | cavity method | bethe lattice | marginal stability\"", "nodeType": "group", "penwidth": "4", "pos": "8188.5,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "12.861" }, { "_gvid": 503, "name": "group2015201729", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 103 | 167 | 269 | 351\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2015", "gid": "group2015201729", "height": "10.986", "label": "
MEAN-FIELD MODEL | EXACT SOLUTION ( 2015 , 2017 ) (((2015,2017),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mean-field model<\/TD> exact solution<\/TD> spatial dimensions<\/TD> hard spheres<\/TD><\/TR>\n
jamming transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | exact solution | spatial dimensions | hard spheres | jamming transition\"", "nodeType": "group", "penwidth": "4", "pos": "20748,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "10.986" }, { "_gvid": 504, "name": "group20152017210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"72 | 73 | 126 | 300 | 386 | 418 | 426\"", "frequence": "\"1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2015", "gid": "group20152017210", "height": "13.292", "label": "
ENTANGLEMENT ENTROPY | ENTANGLEMENT SPECTRUM ( 2015 , 2017 ) (((2015,2017),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
entanglement entropy<\/TD> entanglement spectrum<\/TD> density matrix<\/TD> localization<\/TD><\/TR>\n
thermodynamical limit<\/TD> transition<\/TD> correlation length<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation length | transition | thermodynamical limit | localization | density matrix | entanglement spectrum | entanglement entropy\"", "nodeType": "group", "penwidth": "4", "pos": "22920,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "13.292" }, { "_gvid": 505, "name": "group20152017211", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"76 | 77 | 96 | 126 | 136\"", "frequence": "\"0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2015", "gid": "group20152017211", "height": "11.639", "label": "
THERMODYNAMICAL LIMIT | EQUILIBRIUM ( 2015 , 2017 ) (((2015,2017),2),11)<\/TD><\/TR>\n
<\/TD><\/TR>\n
thermodynamical limit<\/TD> equilibrium<\/TD> critical temperature<\/TD> disordered systems<\/TD><\/TR>\n
ising spin-glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical temperature | disordered systems | equilibrium | thermodynamical limit | ising spin-glasses\"", "nodeType": "group", "penwidth": "4", "pos": "12590,6091.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "11.639" }, { "_gvid": 506, "name": "group20152017212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"87 | 96 | 116 | 136 | 367\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2015", "gid": "group20152017212", "height": "9.7917", "label": "
PROBABILITY DISTRIBUTION | JANUS ( 2015 , 2017 ) (((2015,2017),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
probability distribution<\/TD> janus<\/TD> spin-glass phase<\/TD> equilibrium<\/TD><\/TR>\n
ising spin-glasses<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin-glass phase | equilibrium | probability distribution | ising spin-glasses | janus\"", "nodeType": "group", "penwidth": "4", "pos": "9796.5,6091.5", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2017-10-09\"", "strTo": "\"2017-10-09\"", "support": "1", "to": "2017", "weight": "Just 1.0", "width": "9.7917" }, { "_gvid": 507, "name": "period20162018", "fontsize": "50", "from": "2016", "height": "0.875", "label": "2016 2018", "nodeType": "period", "pos": "33302,5029", "shape": "box", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "to": "2018", "width": "3.9444" }, { "_gvid": 508, "name": "group2016201820", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 23 | 30 | 59 | 97 | 136 | 171 | 225\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2016", "gid": "group2016201820", "height": "9.3333", "label": "
2D | SCALING ( 2016 , 2018 ) (((2016,2018),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
2d<\/TD> scaling<\/TD> zero temperature<\/TD> ising model<\/TD><\/TR>\n
correlation functions<\/TD> field theories<\/TD> ising spin-glasses<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | correlation functions | field theories | zero temperature | ising model | ising spin-glasses | 2d | off-equilibrium dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "9351.5,5029", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "9.3333" }, { "_gvid": 509, "name": "group2016201821", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 193 | 367\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2\"", "from": "2016", "gid": "group2016201821", "height": "7.1944", "label": "
AGING | SCALING ( 2016 , 2018 ) (((2016,2018),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
aging<\/TD> scaling<\/TD> spin glasses<\/TD> janus<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | aging | janus\"", "nodeType": "group", "penwidth": "4", "pos": "6571.5,5029", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "7.1944" }, { "_gvid": 510, "name": "group2016201822", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 254 | 318 | 320\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 0.0 | 0.0\"", "from": "2016", "gid": "group2016201822", "height": "11.556", "label": "
CHAOS | PARALLEL TEMPERING ( 2016 , 2018 ) (((2016,2018),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
chaos<\/TD> parallel tempering<\/TD> finite-dimensional spin glasses<\/TD> spin glasses<\/TD><\/TR>\n
scaling<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | finite-dimensional spin glasses | parallel tempering | chaos\"", "nodeType": "group", "penwidth": "4", "pos": "13586,5029", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "11.556" }, { "_gvid": 511, "name": "group2016201823", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 30 | 54 | 59 | 73 | 87 | 127 | 132 | 143 | 151 | 231 | 317 | 431\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2\"", "from": "2016", "gid": "group2016201823", "height": "11.514", "label": "
BETHE SOLUTION | PHYSICAL MEANING ( 2016 , 2018 ) (((2016,2018),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
bethe solution<\/TD> bray<\/TD> physical meaning<\/TD> finite connectivity<\/TD><\/TR>\n
topology<\/TD> spin-glass model<\/TD> field theories<\/TD> expansion<\/TD><\/TR>\n
zero temperature<\/TD> spin-glass phase<\/TD> spin glasses<\/TD> transition<\/TD><\/TR>\n
bethe lattice<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | field theories | spin glasses | zero temperature | transition | spin-glass phase | topology | spin-glass model | physical meaning | finite connectivity | bray | bethe lattice | bethe solution\"", "nodeType": "group", "penwidth": "4", "pos": "7848.5,5029", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "11.514" }, { "_gvid": 512, "name": "group2016201825", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 54 | 70 | 96 | 100 | 135 | 167 | 304 | 350 | 429\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2016", "gid": "group2016201825", "height": "13.583", "label": "
LARGE DEVIATIONS | EDWARDS-ANDERSON MODEL ( 2016 , 2018 ) (((2016,2018),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
large deviations<\/TD> edwards-anderson model<\/TD> lower critical dimension<\/TD> magnetic field<\/TD><\/TR>\n
spin glasses<\/TD> mean field theory<\/TD> equilibrium<\/TD> fluctuations<\/TD><\/TR>\n
free energy barriers<\/TD> spatial dimensions<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | spin glasses | magnetic field | equilibrium | fluctuations | lower critical dimension | spatial dimensions | edwards-anderson model | large deviations | free energy barriers\"", "nodeType": "group", "penwidth": "4", "pos": "12610,5029", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "13.583" }, { "_gvid": 513, "name": "group2016201826", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 331 | 351 | 387\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2016", "gid": "group2016201826", "height": "11.417", "label": "
INFINITE DIMENSIONS | MEAN FIELD THEORY ( 2016 , 2018 ) (((2016,2018),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
infinite dimensions<\/TD> mean field theory<\/TD> jamming transition<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | infinite dimensions | jamming transition | jamming\"", "nodeType": "group", "penwidth": "4", "pos": "18930,5029", "role": "\"3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "11.417" }, { "_gvid": 514, "name": "group2016201827", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"63 | 73 | 154 | 236 | 315 | 342\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2016", "gid": "group2016201827", "height": "9.8889", "label": "
MEAN-FIELD MODEL | PACKINGS ( 2016 , 2018 ) (((2016,2018),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
mean-field model<\/TD> packings<\/TD> soft spheres<\/TD> random graph<\/TD><\/TR>\n
transition<\/TD> cavity method<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean-field model | transition | random graph | soft spheres | cavity method | packings\"", "nodeType": "group", "penwidth": "4", "pos": "23830,5029", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "9.8889" }, { "_gvid": 515, "name": "group2016201828", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 140 | 189 | 325\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0\"", "from": "2016", "gid": "group2016201828", "height": "14.222", "label": "
RANDOM-LINK MATCHING PROBLEM | FINITE-SIZE CORRECTIONS ( 2016 , 2018 ) (((2016,2018),2),8)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random-link matching problem<\/TD> finite-size corrections<\/TD> matching problem<\/TD> replica approach<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | matching problem | finite-size corrections | random-link matching problem\"", "nodeType": "group", "penwidth": "4", "pos": "25436,5029", "role": "\"3.0 | 2.0 | 3.0 | 1.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2018-10-09\"", "strTo": "\"2018-10-09\"", "support": "1", "to": "2018", "weight": "Just 1.0", "width": "14.222" }, { "_gvid": 516, "name": "period20172019", "fontsize": "50", "from": "2017", "height": "0.875", "label": "2017 2019", "nodeType": "period", "pos": "33302,3950.5", "shape": "box", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "to": "2019", "width": "3.9444" }, { "_gvid": 517, "name": "group2017201920", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 23 | 66 | 77 | 167 | 188\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2017", "gid": "group2017201920", "height": "12.236", "label": "
SUPERSYMMETRY | CORRELATION FUNCTIONS ( 2017 , 2019 ) (((2017,2019),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
supersymmetry<\/TD> correlation functions<\/TD> scaling<\/TD> random-field ising model<\/TD><\/TR>\n
spatial dimensions<\/TD> disordered systems<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | correlation functions | supersymmetry | disordered systems | spatial dimensions | random-field ising model\"", "nodeType": "group", "penwidth": "4", "pos": "15778,3950.5", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "12.236" }, { "_gvid": 518, "name": "group2017201921", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 31 | 54 | 67 | 136 | 141 | 171 | 225 | 238 | 349 | 419\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2017", "gid": "group2017201921", "height": "13.264", "label": "
CRITICAL DYNAMICS | EQUILIBRIUM BEHAVIOR ( 2017 , 2019 ) (((2017,2019),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
critical dynamics<\/TD> spin-glass dynamics<\/TD> equilibrium behavior<\/TD> finite-size effect<\/TD><\/TR>\n
2d<\/TD> scaling<\/TD> ising spin-glasses<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
spin glasses<\/TD> critical points<\/TD> divergence<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | divergence | spin glasses | critical points | ising spin-glasses | finite-size effect | 2d | off-equilibrium dynamics | equilibrium behavior | spin-glass dynamics | critical dynamics\"", "nodeType": "group", "penwidth": "4", "pos": "10530,3950.5", "role": "\"3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "13.264" }, { "_gvid": 519, "name": "group2017201922", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 36 | 90 | 386 | 407 | 414 | 426\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2017", "gid": "group2017201922", "height": "10.5", "label": "
SCALING | RENORMALISATION ( 2017 , 2019 ) (((2017,2019),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
scaling<\/TD> renormalisation<\/TD> ground state<\/TD> entanglement entropy<\/TD><\/TR>\n
hierarchical model<\/TD> density matrix<\/TD> criticality<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | ground state | renormalisation | density matrix | criticality | hierarchical model | entanglement entropy\"", "nodeType": "group", "penwidth": "4", "pos": "21790,3950.5", "role": "\"3.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "10.5" }, { "_gvid": 520, "name": "group2017201924", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 57 | 63 | 67 | 137 | 149 | 184 | 186 | 214 | 237 | 248 | 258 | 334 | 387 | 388 | 407 | 421\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2017", "gid": "group2017201924", "height": "10.681", "label": "
CRYSTALS | EMERGENCE ( 2017 , 2019 ) (((2017,2019),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
crystals<\/TD> analytical solution<\/TD> emergence<\/TD> thermodynamics<\/TD><\/TR>\n
scaling<\/TD> universality class<\/TD> phase diagram<\/TD> free-energy landscape<\/TD><\/TR>\n
specific heat<\/TD> critical points<\/TD> mean-field model<\/TD> marginal stability<\/TD><\/TR>\n
structural glasses<\/TD> power law<\/TD> jamming<\/TD> amorphous solids<\/TD><\/TR>\n
criticality<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | specific heat | mean-field model | critical points | thermodynamics | phase diagram | power law | free-energy landscape | emergence | analytical solution | universality class | structural glasses | amorphous solids | jamming | crystals | criticality | marginal stability\"", "nodeType": "group", "penwidth": "4", "pos": "19856,3950.5", "role": "\"3.0 | 2.0 | 2.0 | 3.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "10.681" }, { "_gvid": 521, "name": "group2017201925", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 57 | 188 | 437 | 438\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2017", "gid": "group2017201925", "height": "9.0833", "label": "
HYPERSCALING RELATION | 5D ( 2017 , 2019 ) (((2017,2019),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hyperscaling relation<\/TD> 5d<\/TD> specific heat<\/TD> critical exponents<\/TD><\/TR>\n
random-field ising model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | specific heat | random-field ising model | 5d | hyperscaling relation\"", "nodeType": "group", "penwidth": "4", "pos": "6450.5,3950.5", "role": "\"3.0 | 2.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2,0.30000000000000004,0.4,0.5,0.6,0.7,0.7999999999999999,0.8999999999999999,0.9999999999999999]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "9.0833" }, { "_gvid": 522, "name": "group2017201926", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"10 | 23 | 67 | 113 | 127 | 133 | 188 | 263 | 347 | 410 | 441 | 442\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2017", "gid": "group2017201926", "height": "13.736", "label": "
FERROMAGNETISM | BELIEF PROPAGATION ( 2017 , 2019 ) (((2017,2019),2),6)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spatial heterogeneity<\/TD> ferromagnetism<\/TD> sparse random graphs<\/TD> belief propagation<\/TD><\/TR>\n
random field<\/TD> low temperature<\/TD> external field<\/TD> correlation functions<\/TD><\/TR>\n
critical points<\/TD> replica symmetry breaking<\/TD> topology<\/TD> random-field ising model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"external field | correlation functions | critical points | random field | topology | replica symmetry breaking | random-field ising model | low temperature | belief propagation | sparse random graphs | ferromagnetism | spatial heterogeneity\"", "nodeType": "group", "penwidth": "4", "pos": "5556.5,3950.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 1.0 | 3.0 | 0.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "13.736" }, { "_gvid": 523, "name": "group2017201927", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"10 | 54 | 87 | 100 | 186 | 263 | 318 | 406\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2017", "gid": "group2017201927", "height": "12.028", "label": "
SPIN-GLASS SIMULATION | PARALLEL TEMPERING ( 2017 , 2019 ) (((2017,2019),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass simulation<\/TD> parallel tempering<\/TD> low temperature<\/TD> spin glasses<\/TD><\/TR>\n
free-energy landscape<\/TD> spin-glass phase<\/TD> external field<\/TD> fluctuations<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"external field | spin glasses | spin-glass phase | fluctuations | free-energy landscape | low temperature | parallel tempering | spin-glass simulation\"", "nodeType": "group", "penwidth": "4", "pos": "14654,3950.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "12.028" }, { "_gvid": 524, "name": "group2017201929", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"53 | 64 | 77 | 103 | 138 | 156 | 222 | 258 | 265 | 302 | 331 | 342 | 351 | 411\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2017", "gid": "group2017201929", "height": "12.208", "label": "
GARDNER TRANSITION | SIMPLE GLASSES ( 2017 , 2019 ) (((2017,2019),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
gardner transition<\/TD> simple glasses<\/TD> metastable states<\/TD> statistical mechanics<\/TD><\/TR>\n
disordered systems<\/TD> complexity<\/TD> mean field theory<\/TD> exact solution<\/TD><\/TR>\n
replica approach<\/TD> infinite dimensions<\/TD> structural glasses<\/TD> statistical physics<\/TD><\/TR>\n
packings<\/TD> jamming transition<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"mean field theory | replica approach | disordered systems | exact solution | statistical mechanics | complexity | metastable states | structural glasses | statistical physics | simple glasses | infinite dimensions | packings | jamming transition | gardner transition\"", "nodeType": "group", "penwidth": "4", "pos": "18960,3950.5", "role": "\"3.0 | 2.0 | 3.0 | 2.0 | 2.0 | 3.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "12.208" }, { "_gvid": 525, "name": "group20172019210", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"54 | 56 | 76 | 87 | 225 | 281 | 301 | 367 | 439 | 440\"", "frequence": "\"5.555555555555558e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2017", "gid": "group20172019210", "height": "12.194", "label": "
MEMORY EFFECT | MPEMBA EFFECT ( 2017 , 2019 ) (((2017,2019),2),10)<\/TD><\/TR>\n
<\/TD><\/TR>\n
memory effect<\/TD> mpemba effect<\/TD> glass formers<\/TD> spin glasses<\/TD><\/TR>\n
spin-glass phase<\/TD> internal energy<\/TD> critical temperature<\/TD> off-equilibrium dynamics<\/TD><\/TR>\n
janus<\/TD> supercooled liquid<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"spin glasses | internal energy | critical temperature | spin-glass phase | off-equilibrium dynamics | glass formers | supercooled liquid | janus | mpemba effect | memory effect\"", "nodeType": "group", "penwidth": "4", "pos": "9203.5,3950.5", "role": "\"3.0 | 2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "12.194" }, { "_gvid": 526, "name": "group20172019212", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"64 | 100 | 117 | 315 | 325 | 372\"", "frequence": "\"0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2017", "gid": "group20172019212", "height": "11.708", "label": "
EXACT EXPRESSION | REPLICAS ( 2017 , 2019 ) (((2017,2019),2),12)<\/TD><\/TR>\n
<\/TD><\/TR>\n
exact expression<\/TD> replicas<\/TD> replica approach<\/TD> random-link matching problem<\/TD><\/TR>\n
fluctuations<\/TD> cavity method<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"replica approach | fluctuations | replicas | cavity method | random-link matching problem | exact expression\"", "nodeType": "group", "penwidth": "4", "pos": "25170,3950.5", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "11.708" }, { "_gvid": 527, "name": "group20172019213", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"124 | 129 | 149 | 150 | 353 | 369 | 386 | 417 | 418 | 436\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2017", "gid": "group20172019213", "height": "12.361", "label": "
RÉNYI ENTROPIES | VON NEUMANN ENTROPY ( 2017 , 2019 ) (((2017,2019),2),13)<\/TD><\/TR>\n
<\/TD><\/TR>\n
rényi entropies<\/TD> von neumann entropy<\/TD> critical line<\/TD> purity<\/TD><\/TR>\n
bipartite entanglement<\/TD> pure states<\/TD> quantum system<\/TD> phase diagram<\/TD><\/TR>\n
entanglement spectrum<\/TD> density matrix<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"quantum system | pure states | phase diagram | critical line | bipartite entanglement | purity | density matrix | von neumann entropy | entanglement spectrum | r\\\\233nyi entropies\"", "nodeType": "group", "penwidth": "4", "pos": "22920,3950.5", "role": "\"2.0 | 2.0 | 3.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2019-10-09\"", "strTo": "\"2019-10-09\"", "support": "1", "to": "2019", "weight": "Just 1.0", "width": "12.361" }, { "_gvid": 528, "name": "period20182020", "fontsize": "50", "from": "2018", "height": "0.875", "label": "2018 2020", "nodeType": "period", "pos": "33302,2857", "shape": "box", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "to": "2020", "width": "3.9444" }, { "_gvid": 529, "name": "group2018202021", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 53 | 54 | 55 | 67 | 76 | 77 | 96 | 117 | 132 | 150 | 189 | 199 | 254 | 261 | 264\"", "frequence": "\"0.0 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2018", "gid": "group2018202021", "height": "14.639", "label": "
LONG-RANGE INTERACTIONS | PARAMAGNETIC PHASE ( 2018 , 2020 ) (((2018,2020),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
long-range interactions<\/TD> paramagnetic phase<\/TD> real replicas<\/TD> equilibrium<\/TD><\/TR>\n
spin glasses<\/TD> spin-glass model<\/TD> finite-dimensional spin glasses<\/TD> critical temperature<\/TD><\/TR>\n
critical line<\/TD> replicas<\/TD> sherrington-kirkpatrick model<\/TD> mean field theory<\/TD><\/TR>\n
critical points<\/TD> phase transition<\/TD> disordered systems<\/TD> finite-size corrections<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | mean field theory | spin glasses | sherrington-kirkpatrick model | critical points | critical temperature | disordered systems | equilibrium | replicas | spin-glass model | critical line | finite-size corrections | real replicas | finite-dimensional spin glasses | paramagnetic phase | long-range interactions\"", "nodeType": "group", "penwidth": "4", "pos": "7986.5,2857", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0 | 2.0 | 3.0 | 2.0 | 3.0 | 3.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "support": "1", "to": "2020", "weight": "Just 1.0", "width": "14.639" }, { "_gvid": 530, "name": "group2018202022", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 17 | 20 | 23 | 25 | 30 | 43 | 48 | 50 | 427 | 449 | 450\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2018", "gid": "group2018202022", "height": "12.264", "label": "
LOOP DIAGRAM | LOOP CALCULATIONS ( 2018 , 2020 ) (((2018,2020),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
loop diagram<\/TD> loop calculations<\/TD> two-loop corrections<\/TD> large-order behavior<\/TD><\/TR>\n
feynman diagram<\/TD> perturbation theory<\/TD> expansion<\/TD> high orders<\/TD><\/TR>\n
quantum field theory<\/TD> field theories<\/TD> correlation functions<\/TD> renormalization group<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | quantum field theory | high orders | correlation functions | perturbation theory | field theories | feynman diagram | renormalization group | large-order behavior | two-loop corrections | loop calculations | loop diagram\"", "nodeType": "group", "penwidth": "4", "pos": "4381.5,2857", "role": "\"3.0 | 2.0 | 2.0 | 3.0 | 1.0 | 3.0 | 2.0 | 2.0 | 3.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "support": "1", "to": "2020", "weight": "Just 1.0", "width": "12.264" }, { "_gvid": 531, "name": "group2018202023", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"14 | 48 | 59 | 65 | 77 | 79 | 152 | 188 | 431\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2\"", "from": "2018", "gid": "group2018202023", "height": "11.819", "label": "
FERROMAGNETS | LOOP EXPANSION ( 2018 , 2020 ) (((2018,2020),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ferromagnets<\/TD> loop expansion<\/TD> random magnetic fields<\/TD> expansion<\/TD><\/TR>\n
zero temperature<\/TD> bethe solution<\/TD> renormalization group<\/TD> disordered systems<\/TD><\/TR>\n
random-field ising model<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"expansion | renormalization group | zero temperature | random magnetic fields | disordered systems | loop expansion | ferromagnets | random-field ising model | bethe solution\"", "nodeType": "group", "penwidth": "4", "pos": "14114,2857", "role": "\"3.0 | 2.0 | 3.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "support": "1", "to": "2020", "weight": "Just 1.0", "width": "11.819" }, { "_gvid": 532, "name": "group2018202024", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 54 | 126 | 193 | 200 | 225 | 237 | 332 | 375 | 394 | 422\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2018", "gid": "group2018202024", "height": "13.917", "label": "
ERGODICITY BREAKING | THEORETICAL MODELS ( 2018 , 2020 ) (((2018,2020),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ergodicity breaking<\/TD> gpus<\/TD> theoretical models<\/TD> out-of-equilibrium dynamics<\/TD><\/TR>\n
mean-field spin glasses<\/TD> spin glasses<\/TD> aging<\/TD> thermodynamical limit<\/TD><\/TR>\n
correlation functions<\/TD> analytical solution<\/TD> off-equilibrium dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | spin glasses | thermodynamical limit | aging | mean-field spin glasses | off-equilibrium dynamics | analytical solution | out-of-equilibrium dynamics | theoretical models | gpus | ergodicity breaking\"", "nodeType": "group", "penwidth": "4", "pos": "6886.5,2857", "role": "\"3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "support": "1", "to": "2020", "weight": "Just 1.0", "width": "13.917" }, { "_gvid": 533, "name": "group2018202025", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"28 | 54 | 70 | 72 | 181 | 367 | 388\"", "frequence": "\"0.0 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0\"", "from": "2018", "gid": "group2018202025", "height": "10.181", "label": "
CORRELATION LENGTH | SPIN GLASSES ( 2018 , 2020 ) (((2018,2020),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
correlation length<\/TD> spin glasses<\/TD> magnetic field<\/TD> crystals<\/TD><\/TR>\n
scaling law<\/TD> janus<\/TD> glassy systems<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling law | spin glasses | magnetic field | correlation length | glassy systems | janus | crystals\"", "nodeType": "group", "penwidth": "4", "pos": "11092,2857", "role": "\"2.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "support": "1", "to": "2020", "weight": "Just 1.0", "width": "10.181" }, { "_gvid": 534, "name": "group2018202027", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"37 | 73 | 236 | 342 | 351 | 387\"", "frequence": "\"1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2018", "gid": "group2018202027", "height": "9.3194", "label": "
SOFT SPHERES | TRANSITION ( 2018 , 2020 ) (((2018,2020),2),7)<\/TD><\/TR>\n
<\/TD><\/TR>\n
soft spheres<\/TD> transition<\/TD> packings<\/TD> jamming transition<\/TD><\/TR>\n
jamming<\/TD> energy<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"energy | transition | soft spheres | packings | jamming transition | jamming\"", "nodeType": "group", "penwidth": "4", "pos": "22508,2857", "role": "\"3.0 | 3.0 | 2.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "support": "1", "to": "2020", "weight": "Just 1.0", "width": "9.3194" }, { "_gvid": 535, "name": "group2018202029", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"127 | 189 | 315 | 325 | 333 | 420\"", "frequence": "\"0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0\"", "from": "2018", "gid": "group2018202029", "height": "13.153", "label": "
RANDOM REGULAR GRAPHS | CAVITY APPROACH ( 2018 , 2020 ) (((2018,2020),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
random regular graphs<\/TD> cavity approach<\/TD> random-link matching problem<\/TD> cavity method<\/TD><\/TR>\n
finite-size corrections<\/TD> topology<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"topology | finite-size corrections | cavity method | random-link matching problem | cavity approach | random regular graphs\"", "nodeType": "group", "penwidth": "4", "pos": "25436,2857", "role": "\"2.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2020-10-09\"", "strTo": "\"2020-10-09\"", "support": "1", "to": "2020", "weight": "Just 1.0", "width": "13.153" }, { "_gvid": 536, "name": "period20192021", "fontsize": "50", "from": "2019", "height": "0.875", "label": "2019 2021", "nodeType": "period", "pos": "33302,1713.5", "shape": "box", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "to": "2021", "width": "3.9444" }, { "_gvid": 537, "name": "group2019202120", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 5 | 92 | 134 | 141 | 145 | 167 | 248 | 334 | 342 | 387 | 390 | 397 | 407 | 412 | 456\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2019", "gid": "group2019202120", "height": "10.681", "label": "
COLLOIDS | SCALING ( 2019 , 2021 ) (((2019,2021),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
colloids<\/TD> scaling<\/TD> jammed configurations<\/TD> jamming point<\/TD><\/TR>\n
critical properties<\/TD> universality class<\/TD> disorder<\/TD> isostaticity<\/TD><\/TR>\n
jamming<\/TD> amorphous solids<\/TD> spatial dimensions<\/TD> theoretical predictions<\/TD><\/TR>\n
finite-size effect<\/TD> neural network<\/TD> packings<\/TD> criticality<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | theoretical predictions | critical properties | disorder | finite-size effect | neural network | spatial dimensions | universality class | amorphous solids | packings | jamming | colloids | jamming point | criticality | isostaticity | jammed configurations\"", "nodeType": "group", "penwidth": "4", "pos": "19856,1713.5", "role": "\"3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "support": "1", "to": "2021", "weight": "Just 1.0", "width": "10.681" }, { "_gvid": 538, "name": "group2019202121", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 37 | 54 | 73 | 82 | 87 | 149 | 156 | 261 | 273 | 345 | 349 | 457 | 458 | 459 | 460 | 461 | 462 | 463\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2019", "gid": "group2019202121", "height": "13.389", "label": "
HOPFIELD-LIKE SYSTEM | METROPOLIS ALGORITHM ( 2019 , 2021 ) (((2019,2021),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
hopfield-like system<\/TD> metropolis algorithm<\/TD> social systems<\/TD> tunable complexity<\/TD><\/TR>\n
potential energy landscape<\/TD> computer science<\/TD> spin glasses<\/TD> spin models<\/TD><\/TR>\n
optical computation<\/TD> transition<\/TD> complexity<\/TD> scaling<\/TD><\/TR>\n
paramagnetic phase<\/TD> paradigmatic models<\/TD> spin-glass phase<\/TD> energy<\/TD><\/TR>\n
phase diagram<\/TD> optical simulation<\/TD> spin-glass dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | energy | spin glasses | transition | spin models | spin-glass phase | phase diagram | complexity | paramagnetic phase | potential energy landscape | computer science | spin-glass dynamics | optical computation | tunable complexity | paradigmatic models | social systems | optical simulation | metropolis algorithm | hopfield-like system\"", "nodeType": "group", "penwidth": "4", "pos": "4952.5,1713.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 3.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "support": "1", "to": "2021", "weight": "Just 1.0", "width": "13.389" }, { "_gvid": 539, "name": "group2019202122", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 54 | 70 | 72 | 225 | 349 | 367 | 370 | 388 | 395 | 476\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 0.0 | 0.0 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0\"", "from": "2019", "gid": "group2019202122", "height": "12.569", "label": "
ZEEMAN ENERGY | MICROSCOPIC PROPERTIES ( 2019 , 2021 ) (((2019,2021),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
zeeman energy<\/TD> microscopic properties<\/TD> spin-glass transition<\/TD> spin glasses<\/TD><\/TR>\n
correlation length<\/TD> magnetic field<\/TD> janus<\/TD> crystals<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> scaling<\/TD> spin-glass dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | spin glasses | magnetic field | correlation length | off-equilibrium dynamics | spin-glass dynamics | janus | spin-glass transition | crystals | microscopic properties | zeeman energy\"", "nodeType": "group", "penwidth": "4", "pos": "10530,1713.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 2.0 | 2.0 | 3.0 | 3.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "support": "1", "to": "2021", "weight": "Just 1.0", "width": "12.569" }, { "_gvid": 540, "name": "group2019202123", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"6 | 15 | 73 | 92 | 269 | 351 | 464 | 465 | 466 | 467 | 468\"", "frequence": "\"0.0 | 0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2019", "gid": "group2019202123", "height": "15.125", "label": "
ULTRALOW TEMPERATURES | QUANTUM CRITICAL POINTS ( 2019 , 2021 ) (((2019,2021),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ultralow temperatures<\/TD> quantum critical points<\/TD> quantum dynamics<\/TD> quantum mechanical perceptron<\/TD><\/TR>\n
quantum jamming<\/TD> critical exponents<\/TD> euclidean space<\/TD> hard spheres<\/TD><\/TR>\n
jamming transition<\/TD> transition<\/TD> critical properties<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"critical exponents | euclidean space | transition | critical properties | hard spheres | jamming transition | quantum jamming | quantum mechanical perceptron | quantum dynamics | quantum critical points | ultralow temperatures\"", "nodeType": "group", "penwidth": "4", "pos": "21802,1713.5", "role": "\"2.0 | 2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "support": "1", "to": "2021", "weight": "Just 1.0", "width": "15.125" }, { "_gvid": 541, "name": "group2019202124", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"11 | 73 | 91 | 113 | 133 | 149 | 150 | 261 | 410 | 441\"", "frequence": "\"0.0 | 3.7037037037037056e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2019", "gid": "group2019202124", "height": "13.153", "label": "
FERROMAGNETISM | SPARSE RANDOM GRAPHS ( 2019 , 2021 ) (((2019,2021),2),4)<\/TD><\/TR>\n
<\/TD><\/TR>\n
ferromagnetism<\/TD> sparse random graphs<\/TD> replica symmetry breaking<\/TD> random field<\/TD><\/TR>\n
paramagnetic phase<\/TD> critical line<\/TD> phase transition<\/TD> transition<\/TD><\/TR>\n
first-order transitions<\/TD> phase diagram<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"phase transition | transition | first-order transitions | random field | replica symmetry breaking | phase diagram | critical line | paramagnetic phase | sparse random graphs | ferromagnetism\"", "nodeType": "group", "penwidth": "4", "pos": "6692.5,1713.5", "role": "\"2.0 | 3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "support": "1", "to": "2021", "weight": "Just 1.0", "width": "13.153" }, { "_gvid": 542, "name": "group2019202125", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 78 | 100 | 269 | 377 | 387 | 401 | 412 | 452 | 453 | 454 | 455\"", "frequence": "\"1.8518518518518528e-2 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "from": "2019", "gid": "group2019202125", "height": "14.278", "label": "
ANOMALOUS LONG-RANGE DECAY | ΔZ FLUCTUATIONS ( 2019 , 2021 ) (((2019,2021),2),5)<\/TD><\/TR>\n
<\/TD><\/TR>\n
anomalous long-range decay<\/TD> δz fluctuations<\/TD> weak forces<\/TD> anomalous decay<\/TD><\/TR>\n
jammed packings<\/TD> large-scale behavior<\/TD> three-dimensional systems<\/TD> correlation functions<\/TD><\/TR>\n
hard spheres<\/TD> isostaticity<\/TD> fluctuations<\/TD> jamming<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | three-dimensional systems | fluctuations | hard spheres | large-scale behavior | jamming | jammed packings | isostaticity | anomalous decay | weak forces | \\\\948z fluctuations | anomalous long-range decay\"", "nodeType": "group", "penwidth": "4", "pos": "17354,1713.5", "role": "\"3.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "support": "1", "to": "2021", "weight": "Just 1.0", "width": "14.278" }, { "_gvid": 543, "name": "group2019202129", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"96 | 181 | 225 | 304 | 319 | 320 | 349 | 367 | 428 | 435\"", "frequence": "\"0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 1.8518518518518528e-2 | 0.0 | 0.0\"", "from": "2019", "gid": "group2019202129", "height": "12.139", "label": "
SPIN-GLASS COHERENCE | CHAOS ( 2019 , 2021 ) (((2019,2021),2),9)<\/TD><\/TR>\n
<\/TD><\/TR>\n
spin-glass coherence<\/TD> chaos<\/TD> temperature chaos<\/TD> glassy systems<\/TD><\/TR>\n
off-equilibrium dynamics<\/TD> edwards-anderson model<\/TD> spatially heterogeneous<\/TD> equilibrium<\/TD><\/TR>\n
janus<\/TD> spin-glass dynamics<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"equilibrium | glassy systems | off-equilibrium dynamics | edwards-anderson model | temperature chaos | chaos | spin-glass dynamics | janus | spin-glass coherence | spatially heterogeneous\"", "nodeType": "group", "penwidth": "4", "pos": "12610,1713.5", "role": "\"2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 2.0 | 3.0 | 2.0 | 2.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2021-10-09\"", "strTo": "\"2021-10-09\"", "support": "1", "to": "2021", "weight": "Just 1.0", "width": "12.139" }, { "_gvid": 544, "name": "period20202022", "fontsize": "50", "from": "2020", "height": "0.875", "label": "2020 2022", "nodeType": "period", "pos": "33302,548.5", "shape": "box", "strFrom": "\"2022-10-09\"", "strTo": "\"2022-10-09\"", "to": "2022", "width": "3.9444" }, { "_gvid": 545, "name": "group2020202220", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"4 | 37 | 54 | 59 | 67 | 69 | 73 | 87 | 126 | 132 | 261 | 315 | 370 | 407 | 480 | 481 | 482 | 483\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2020", "gid": "group2020202220", "height": "15.236", "label": "
DELOCALIZATION | QUASI-LOCALIZATION PROPERTIES ( 2020 , 2022 ) (((2020,2022),2),0)<\/TD><\/TR>\n
<\/TD><\/TR>\n
delocalization<\/TD> quasi-localization properties<\/TD> low energy excitation modes<\/TD> delocalization transition<\/TD><\/TR>\n
spin glasses<\/TD> spin-glass phase<\/TD> external magnetic field<\/TD> scaling<\/TD><\/TR>\n
spin-glass model<\/TD> zero temperature<\/TD> spin-glass transition<\/TD> energy<\/TD><\/TR>\n
transition<\/TD> thermodynamical limit<\/TD> cavity method<\/TD> critical points<\/TD><\/TR>\n
paramagnetic phase<\/TD> criticality<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"scaling | energy | spin glasses | zero temperature | critical points | external magnetic field | transition | spin-glass phase | thermodynamical limit | spin-glass model | paramagnetic phase | cavity method | spin-glass transition | criticality | delocalization transition | low energy excitation modes | quasi-localization properties | delocalization\"", "nodeType": "group", "penwidth": "4", "pos": "7986.5,548.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0 | 0.0 | 0.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2022-10-09\"", "strTo": "\"2022-10-09\"", "support": "1", "to": "2022", "weight": "Just 1.0", "width": "15.236" }, { "_gvid": 546, "name": "group2020202221", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"10 | 14 | 53 | 54 | 59 | 73 | 79 | 132 | 151 | 242 | 317 | 370 | 399 | 431 | 479\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 5.555555555555558e-2 | 3.7037037037037056e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2020", "gid": "group2020202221", "height": "14.986", "label": "
FINITE-TEMPERATURE REPLICA FIELD THEORY | GINZBURG CRITERION ( 2020 , 2022 ) (((2020,2022),2),1)<\/TD><\/TR>\n
<\/TD><\/TR>\n
finite-temperature replica field theory<\/TD> ginzburg criterion<\/TD> upper critical dimension<\/TD> finite connectivity<\/TD><\/TR>\n
loop expansion<\/TD> zero temperature<\/TD> spin-glass model<\/TD> spin glasses<\/TD><\/TR>\n
bethe solution<\/TD> expansion<\/TD> transition<\/TD> mean field theory<\/TD><\/TR>\n
spin-glass transition<\/TD> external field<\/TD> bethe lattice<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"external field | expansion | mean field theory | spin glasses | zero temperature | transition | loop expansion | spin-glass model | finite connectivity | upper critical dimension | bethe lattice | spin-glass transition | ginzburg criterion | bethe solution | finite-temperature replica field theory\"", "nodeType": "group", "penwidth": "4", "pos": "14480,548.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2022-10-09\"", "strTo": "\"2022-10-09\"", "support": "1", "to": "2022", "weight": "Just 1.0", "width": "14.986" }, { "_gvid": 547, "name": "group2020202222", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"23 | 25 | 40 | 42 | 50 | 109 | 207 | 427\"", "frequence": "\"1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2020", "gid": "group2020202222", "height": "13.722", "label": "
PERTURBATION THEORY | CORRELATION FUNCTIONS ( 2020 , 2022 ) (((2020,2022),2),2)<\/TD><\/TR>\n
<\/TD><\/TR>\n
perturbation theory<\/TD> correlation functions<\/TD> oscillators<\/TD> partition function<\/TD><\/TR>\n
large-order behavior<\/TD> asymptotic estimates<\/TD> anharmonic oscillator<\/TD> two-loop corrections<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"correlation functions | perturbation theory | anharmonic oscillator | asymptotic estimates | large-order behavior | partition function | oscillators | two-loop corrections\"", "nodeType": "group", "penwidth": "4", "pos": "4361.5,548.5", "role": "\"3.0 | 3.0 | 1.0 | 1.0 | 3.0 | 3.0 | 3.0 | 3.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2022-10-09\"", "strTo": "\"2022-10-09\"", "support": "1", "to": "2022", "weight": "Just 1.0", "width": "13.722" }, { "_gvid": 548, "name": "group2020202223", "bId": "4", "branchId": "0 71 1", "fontname": "Arial", "foundation": "\"30 | 54 | 70 | 72 | 136 | 167 | 231 | 281 | 301 | 317 | 367 | 390 | 478\"", "frequence": "\"1.8518518518518528e-2 | 5.555555555555558e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 3.7037037037037056e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2 | 1.8518518518518528e-2\"", "from": "2020", "gid": "group2020202223", "height": "11.264", "label": "
REPLICA-SYMMETRIC HAMILTONIAN | BRAY ( 2020 , 2022 ) (((2020,2022),2),3)<\/TD><\/TR>\n
<\/TD><\/TR>\n
replica-symmetric hamiltonian<\/TD> bray<\/TD> supercooled liquid<\/TD> glass formers<\/TD><\/TR>\n
ising spin-glasses<\/TD> spin glasses<\/TD> correlation length<\/TD> magnetic field<\/TD><\/TR>\n
spatial dimensions<\/TD> field theories<\/TD> colloids<\/TD> janus<\/TD><\/TR>\n
bethe lattice<\/TD><\/TR><\/TABLE><\/FONT>", "lbl": "\"field theories | spin glasses | magnetic field | correlation length | ising spin-glasses | spatial dimensions | bray | glass formers | supercooled liquid | bethe lattice | janus | colloids | replica-symmetric hamiltonian\"", "nodeType": "group", "penwidth": "4", "pos": "10338,548.5", "role": "\"3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 3.0 | 0.0\"", "seaLvl": "[0.0,0.1,0.2]", "shape": "square", "source": "[]", "sourceFull": "[]", "strFrom": "\"2022-10-09\"", "strTo": "\"2022-10-09\"", "support": "1", "to": "2022", "weight": "Just 1.0", "width": "11.264" } ], "edges": [ { "_gvid": 0, "tail": 52, "head": 59, "arrowhead": "rdot", "color": "black", "edgeType": "branchLink", "pos": "e,1912.1,54764 2381.7,54862 2210.8,54845 2024.3,54818 1947.5,54782 1938,54778 1928.6,54773 1919.2,54768", "width": "3" }, { "_gvid": 1, "tail": 52, "head": 60, "arrowhead": "rdot", "color": "black", "edgeType": "branchLink", "pos": 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