effecve field theory of dissipave fluids
TRANSCRIPT
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Effec%veFieldTheoryofDissipa%veFluids
HongLiu
MichaelCrossleyarXiv:1511.03646andtoappear
PaoloGlorioso
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Conservedquan%%esandhydrodynamics
Considerlongwavelengthdisturbancesofasysteminthermalequilibrium:
conservedquan%%es:cannotrelaxlocally,onlyviatransports
Conservedquan%%esGaplessandlong-livedmodes
Thereshouldexistauniversallowenergyeffec%vetheory.
non-conservedquan%%es:relaxlocally,
Phenomenologicaldescrip%on: Hydrodynamics
(onlyonesinthermalequilibrium)
slowlyvaryingfunc%onsofspace%me
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O’Haraetal(2002)
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Despitethelongandglorioushistoryofhydrodynamics
Itdoesnotcapturefluctua%ons,whicharealwayspresent,andareimportantinmanyphysicalcontexts:
Transports(long%metail),dynamicalaspectsofphasetransi%ons,non-equilibriumsteadystates,turbulence,finitesizesystems….......
Phenomenologicallevel:stochas%chydro(Landau,Lifshitz)
Goodfornear-equilibriumdisturbances(linearized)
Butnotadequateforfar-from-equilibriumsitua%ons
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Rayleigh-Benardproblem
Hydrodynamicfluctua%onshot
cold
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Constraints
Cons%tu%verela%ons:notenoughtojustwritedownthemostgeneralderiva%veexpansionconsistentwithsymmetries.
1.Entropycondi%on
2.Onsagerrela%ons:linearresponsematrixmustbesymmetric
Phenomenologicalconstraints:solu%onsshouldsa%sfy:
Arethesecomplete?
Currentformula%onofhydrodynamicsisawkward.
awkward:usesolu%onstoconstrainequa%onsofmo%on
Microscopicorigin?
Clearlysomethingmorefundamentalismissing
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Willaddresstheseissuesbydevelopinghydrodynamicsasalowenergyeffec%vefieldtheoryofageneralmany-bodysystematfinitetemperature
Ac%onprincipleforfullfluctua%nghydrodynamicsapplicabletofarfromequilibriumsitua%ons
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Closed%mepath
Standardlore:Dissipa%vesystemsdon'thaveanac%onformula%on
Thisissueisnaturallyresolvedbyquantummechanics.
Closed%mepath(CTP)orSchwinger-Keldyshcontour
Interestedindescribingreal-%medynamicsaroundastate,nottransi%onamplitude
Requiresdoublingthenumberofd.o.f.
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Closed%mepath
Standardlore:Dissipa%vesystemsdon'thaveanac%onformula%on
Thisissueisnaturallyresolvedbyquantummechanics.
Closed%mepath(CTP)orSchwinger-Keldyshcontour
Interestedindescribingreal-%medynamicsaroundastate,nottransi%onamplitude
Requiresdoublingthenumberofd.o.f.
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Effec%vefieldtheoryforfluidsMicroscopicdescrip%on(inthermaldensitymatrix)
Macroscopicphenomena
HydroEFT:
RG
donotwork
3.Integra%onmeasure?
• thermalstatereflectedincoefficientsofac%on
• Standardhydro:saddlepointequa%ons
hydrodynamicmodes(2sets)
1.Whatare?
2.Whatarethesymmetriesof?
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Searchingforanac%onprinciplefordissipa%vehydrodynamicshasbeenalongstandingproblem,da%ngbackatleasttotheidealfluidac%onofG.Herglotzin1911.
Relativistic: Taub, Salmon, Carter, …...
Includingdissipa%on:GrozdanovandPolonyi;Harder,Kovtun,andRitz;Kovtun,MooreandRomatschke;Endlich,Nicolis,PortoandJ.Wang,…...
Holographic: Nickel, Son; de Boer, Heller, Pinzani-Fokeeva; Crossley, Glorioso., HL, Y. Wang.
Reviews: Jackiw, Nair,PiandPolychronakos;Andersson and Comer
Dubovsky,Gregoire,NicolisandRaiazzihep-th/0512260
The last decade has seen a renewed interest:
Dubovsky,Hui,NicolisandSon,arXiv:1107.0731
Analterna%veapproach:Haehl,LoganayagamandRangamani,arXiv:1510.02494,1511.07809
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Hereforconceptualsimplicity,Iwilldescribethestoryforneutralnormalfluids.
Descrip%onforfullchargedfluidsisgivenin:
Crossley,Glorioso,andHL,arXiv:1511.03646
Canalsobegeneralizedtosuperfluids(S.RajagopalandHL,toappear)
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DynamicalvariablesRecallLagrangedescrip%onofhydrodynamics:
:labelfluidelements : describefluidmo%on
An”integra%ng-in”proceduretoiden%fygaplessandlong-livedd.o.f.associatedwithaconservedstresstensor:
:internal%me
AlsonaturalfromHolography:Nickel,Son,arXiv:1009.3094
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Standardhydrovariables(whicharenowderivedquan%%es)
Noise:
Asignificantchallenge:ensuretheeomsfromtheac%onofXcanbesolelyexpressedintermsofthesevelocity.(e.g.solidsv.s.fluids)
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Symmetries
Requiretheac%ontobeinvariantunder:
labelindividualfluidelements, internal%me
definewhatisafluid!
Itturnsoutthesesymmetriesindeeddomagicforyou:
atthelevelofequa%onsofmo%on,theyensurealldependenceondynamicalvariablescanbeexpressedinandtemperature.
Recoverstandardformula%onofhydrodynamics(modulophenomenologicalconstraints)
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Thiswouldbethefullthestoryinausualsitua%on.
Fullnon-linearfluidfluctua%ngdynamicsencodedinnon-trivialdifferen%algeometry:
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Consistencycondi%onsandsymmetries
ForasystemdefinedwithCTP:
constraintsoncorrela%onfunc%ons,
Requirefurthersymmetriessa%sfiedbytheoff-shellac%onsothattheseconstraintcondi%onsaresa%sfiedaoerdoingthepathintegral.
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g1
g2=
Reflec%vityandKMScondi%ons
Canbesa%sfiedbyimposingaZ2reflec%onsymmetryonbothdynamicalandbackgroundfields
Complexac%on:non-nega%vityofimaginarypart
• KMScondi%onsplusCPTimplyaZ2symmetryonW:
inversetemperatureatspa%alinfini%escharacterizethermalstateCanbesa%sfiedbyimposingaZ2symmetryontheac%on:localKMScondi%ons
• Reflec%vitycondi%on:
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• Non-equilibriumfluctua%on-dissipa%onrela%ons
• Alltheconstraintsfromentropycurrentcondi%onandlinearOnsagerrela%ons
• Newconstraintsonequa%onsofmo%onfromnonlineargeneraliza%onsofOnsagerrela%ons.
Crossley,Glorioso,HLtoappear
LocalZ2KMScondi%on+equa%onsofmo%on+non-nega%vityofimaginarypartoftheac%on
conservedandentropycurrentatideallevel
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Unitarycondi%on
Thismaybeconsideredasacondi%ononpathintegralmeasure.
Todescribehydrodynamicalflucatua%onsproperlyan%-commu%ngobjectsareneeded!
SeealsoHaehl,LoganayagamandRangamaniarXiv:1510.02494
g1=g
g2=g
(BRSTsymmetryhereisaglobalsymmetry)
Resolu%on:Introduceafermionicpartner(“ghost”)foreachdynamicalvariableandrequiretheac%ontohavea“BRST”typesymmetry:
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KMScondi%onandSupersymmetry
SeealsoHaehl,LoganayagamandRangamani,arXiv:1510.02494,1511.07809
Strongindica%onsthatBRST+localKMScondi%on
PingGaoandHL,inprogress
emergentfermionicsymmetry:
Classicallimit: Standardsupersymmetryin%medirec%on.
Quantumlevel:indica%onsofa“quantum-deformed”SUSYalgebra
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Summary1.Hydrodynamicswithclassicalsta%s%calfluctua%onsisdescribedbyasupersymmetricquantumfieldtheory
2.Hydrodynamicswithquantumfluctua%onsalsoincorporated
isdescribedbya“quantum-deformed”(supersymmetric)quantumfieldtheory.
• Recoversthestandardhydrodynamics,newconstraints,non-equilibriumfluctua%on-dissipa%onrela%ons
• Fullnon-linearfluidfluctua%ngdynamicsencodedinnon-trivialdifferen%algeometry.
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Bosonicac%onforfullchargedfluidsAdoubleexpansionintermsofnoisesandderiva%ves:
Allcoefficientsarefunc%onsof
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Futuredirec%onsFormalism:
Non-rela%vis%c,(toappearwithGlorioso)
Applica%ons:
Transports(long%metails)
Dynamicalaspectsofphasetransi%ons
NovelfixedpointsofhydroEFT,suchasKPZscaling,turbulence….
….........
Non-equilibriumsteadystates,dynamicalflowsofQGP
“quantum-deformed”Supersymmetry…....
superfluids,(toappearwithS.Rajagopal)
DeeperunderstandingofKMS,unitarityandsupersymmetry(inprogresswithPingGao)
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Thankyou!