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1、TheoryofMany-ParticleSystemsLecturenotesforP654,CornellUniversity,spring2005.cPietBrouwer,2005.Permissionisgrantedtoprintandcopythesenotes,ifkepttogetherwiththetitlepageandthiscopyrightnotice.Chapter1Preliminaries1.1ThermalaverageIntheliterature,twotypesoftheoriesareconst
2、ructedtodescribeasystemofmanyparticles:Theoriesofthemany-particlegroundstate,andtheoriesthataddressathermalaverageattemperatureT.Inthiscourse,we'lllimitourselvestonite-temperaturethermalequilibriaandtononequilibriumsituationsthatarisefromanite-temperatureequilibriumbysw
3、itch-ingonatime-dependentperturbationintheHamiltonian.Inallcasesofinteresttous,resultsatzerotemperaturecanbeobtainedasthezerotemperaturelimitofthenite-temperaturetheory.Below,webrie
yrecallthebasicresultsofequilibriumstatisticalmechanics.ThethermalaverageofanobservableAi
4、sdenedashAi=trA^;^(1.1)where^isthedensitymatrixandA^istheoperatorcorrespondingtotheobservableA.Thedensitymatrix^describesthethermaldistributionoverthedierenteigenstatesofthesystem.Thesymboltrdenotesthetrace"ofanoperator,thesummationovertheexpectationvaluesoftheopera
5、toroveranorthonormalbasisset,XtrA=hnjAjni:(1.2)nThebasissetfjnigcanbethecollectionofmany-particleeigenstatesoftheHamiltonianH^,oranyotherorthonormalbasisset.Inthecanonicalensembleofstatisticalmechanics,thetraceistakenoverallstateswithNparticlesandonehas1 H^=T H^=T^=e;Z
6、=tre;(1.3)Z12CHAPTER1.PRELIMINARIESwhereH^istheHamiltonian.UsingthebasisofN-particleeigenstatesjnioftheHamiltonianH^,witheigenvaluesEn,thethermalaveragehAicanthenbewrittenasPe En=ThnjA^jnihAi=nP:(1.4)e En=TnInthegrand-canonicalensemble,thetraceistakenoverallstates,irrespe
7、ctiveofparticlenumber,andonehas1 (H^ N^)=T (H^ N^)=T=e;Z=tre:(1.5)ZHereisthechemicalpotentialandNistheparticlenumberoperator.Usuallywewillincludetheterm N^intothedenitionoftheHamiltonianH^,sothatexpressionsforthethermalaverageinthecanonicalandgrandcanonicalensembles
8、areformallyidentical.1.2Schr•odinger,Heisenberg,andinteractionpictureThereexistformallydierentb