on the static and dynamical transition in the

on the static and dynamical transition in the

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时间:2019-03-06

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1、Figure12:Energyversustemperatureincasep=40,J=?18.Thecontinuouslineis0theone-stepsolution.Thedashedlineisthehigh-Tresult.ThetransitiontemperaturesareT'1:71;T'1:76.ThecrossesandthefullsquarescorrespondtotheGaussianRSBGmodelwithN=1000andtwodi erentsamples.34Figure11:Ener

2、gyversustemperatureincasep=20,J=?8.Thecontinuouslineis0theone-stepsolution.Thedashedlineisthehigh-Tresult.ThetransitiontemperaturesareT'1:36;T'1:39.ThecrossesandthefulldotscorrespondtotheGaussianRSBGmodelwithN=2000andtwocoolingprocedures(thesimulationswithcrossesare10

3、timeslargerinsimulationtimethanthedots).33Figure10:Energyversustemperatureincasep=10,J=?3.Thecontinuouslineisthe0one-stepsolution.Thedashedlineisthehigh-Tresult.ThetransitiontemperaturesareT'1:13;T'1:14.ThefulldotsaresimulationresultsforN=1000.RSBG32Figure9:Energyvers

4、ustemperatureincasep=5,J=?1.Thecontinuouslineisthe0one-stepsolution.Thedashedlineisthehigh-Tresult.ThetransitiontemperaturesareT'1:0091;T'1:01.ThefulldotsaresimulationresultsforN=1000.RSBG31Figure8:Energyversustemperatureincasep=3,J=0.Thecontinuouslineisthe0one-stepso

5、lution.Thedashedlineisthehigh-Tresult.ThetransitiontemperatureisT=T=1.ThefulldotsareforonesampleandN=2000.RSBG30Figure7:Probabilitydistributionofthemagnetizationassociatedtothezero-temperaturemetastablestates.Thesingularityatm=?1meansthatonlysomestatesarepopulated.The

6、sameparametersasin gure6.29Figure6:Probabilitydistributionoftheenergyofthegroundstatesforcasep=10andJ=0andN=100.028Figure5:Magneticsusceptibilityversustemperatureforthecasep=10withJ=0.The0 rstpeakappearsatT2:3.F27Figure4:Energyversustemperatureforthecasep=10withJ=0.T

7、hecontinuousline0correspondstotheonestepspin-glasssolutionandthedashedlineisthehigh-Tresult.Theferromagnetictransitioniscloseto2:3.SimulationresultsareforonesampleandN=1000.261Figure3:ThestaticandthedynamicEdwards-Andersonparameterasafunctionof.log(p)Theyincreaselogar

8、ithmicallywithp.Thedotsareforthestaticvalue,thecrossesforthedynamicalone.25Figure2:Theone-stepbreakingparametermasafunctiono

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