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1、ExploringReal-timeFunctionsontheLatticewithInversePropagatorandSelf-EnergyMasakiyoKitazawa(OsakaU.)22/Sep./2011LunchSeminar@BNLQCD@T>0TRHICLHCperturbationLatticeQCDHowdoesthematterbehaveinthisregion?Tc*QuantumStatisticalMechanicsStaticexpectationvalueDynamicalresponseEoSch
2、iralcondensatesusceptibilitiesscreeningmass…Spectralfunc:SpectralFunctionsatT>0quasi-particleexcitationwidth~decayratetransportcoefficientsr(w,p)wpeaksKuboformulaeslopeattheoriginshearviscosity:T12bulkviscosity:Tmmelectricconductivity:JiiAnalyticContinuationanalyticcontinua
3、tionRetarded(real-time)propagatorSpectralfunctionImaginary-time(Matsubara)propagatorLatticeDynamicsAnalyticContinuationMEManalysisofr(w)mostprobableimageestimatedbylatticedata+priorknowledgeAsakawa,Hatsuda,Nakahara,1999qualitativestructureofr(w)Asakawa,Hatsuda,2004;Datta,eta
4、l.,2004;…LatticeDynamicsAnalyticContinuationQuestions:Arethereotherusefulformulastorelatereal-timeandEuclideanfunctions?Isr(w)onlyareal-timefunctionworthanalyzing?Weconsidertheinversepropagator.cf.)sumrulesKharzeev,Tuchin;Karsch,Kharzeev,Tuchin,2008Romatchke,Son,2009;Meyer,2
5、010;…ADifficultyinAnalyzingLowEnergySpectrumMomentExpansionTaylorexpandcoshw(t-1/2T)momentof“thermal”spectrumCnn-thmomentofr’(w).Aarts,etal.,2002Petreczky,Teany,2006Ding,2010LowEnergySpectrumLwContributionofhigherordermomentsoflowenergypartisseverelysuppressed.ForL=T,thera
6、tiois2.1x10-5forn=6.InversePropagatorandAnalyticContinuationInversePropagatorLatticeobservableDynamicalinformationanalyticinverseanalyticinverseF.T.F.T.inverseNumericalProcedureLatticeobservableDynamicalinformationinverseinverseStandardanalysisPresentstudyTranslationalsymmet
7、ryreducescostsfortheinverse.[S]-1(t)isnotthestatisticalaverageoffermionmatrix.F.T.Inv.F.T.QuarkSelf-Energydecayrateofquasi-quark@poleTheoretically,ImSisusefultounderstandspectralproperties.experimentalobservableSpectralfunctionSelf-energy(ImS)Im.partToInterpretPhysicsbehindt
8、heSPCphysicalinterpretationviaopticaltheoremDisp.Rel.wwwSelf-EnergyforDiscr