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Softhairsonisolatedhorizonimplantedbyelectromagneticfields
InspiredbytherecentproposalofsofthaironblackholesinHawkingetal(2016Phys.Rev.Lett.116231301),wehaveshownthatanisolatedhorizoncarriessofthairsimplantedbyelectromagneticfields.ThesolutionspaceandtheasymptoticsymmetriesofEinstein–Maxwelltheoryhavebeenworkedoutexplicitlyneartheisolatedhorizon.TheconservedcurrenthasbeencomputedandaninfinitenumberofnearhorizonchargeshavebeenintroducedfromtheelectromagneticfieldsassociatedwiththeasymptoticU(1)symmetrynearthehorizon,whichindicatesthefactthattheisolatedhorizoncarriesalargeamountofsoftelectrichairs.Thesoftelectrichairs,i.e.asymptoticU(1)charges,areshowntobeequivalenttotheelectricmultipolemomentsofisolatedhorizons.Itisfurtherarguedthattheisolatedhorizonsupertranslationisfromtheambiguityofitsfoliationandananalogueofmemoryeffectonhorizoncanbeexpected.
FromPrigoginetoRaychaudhuri
ItishighlightedbyPrigoginethattherearetwoadditionaluniversalbehaviorsassociatedwiththeentropyproductionratebesidesthefourlawsofthermodynamics.Oneisthattheentropyproductionratedecreaseswhenthesystemapproachesthesteadystate,andtheotheristhattheentropyproductionratereachesitsminimalvalueatthesteadystate.MotivatedbytheblackholethermodynamicsandAdS/CFTcorrespondence,weresorttotheRaychaudhuriequationtoprovethatthesetwouniversalbehaviorsarealsoobeyedbytheblackholeentropy.Inparticular,ourresulttogetherwiththefourlawsofblackholethermodynamicsfurtherindicatesthattheholographicgravityshouldbeuniversal,notrestrictedonlywithinthecontextofAdS/CFTcorrespondence.
Holographicinterpretationofacousticblackholes
Withtheattempttofindtheholographicdescriptionoftheusualacousticblackholesinfluid,weconstructanacousticblackholeformedinthed-dimensionalfluidlocatedatthetimelikecutoffsurfaceofaneutralblackbraneinasymptoticallyAdSd+1spacetime.
Fluid/gravitycorrespondenceforgeneralnon-rotatingblackholes
Inthispaper,weinvestigatethefluid/gravitycorrespondenceinspacetimewithgeneralnon-rotatingweaklyisolatedhorizon.WiththehelpofaPetrov-likeboundaryconditionandlargemeancurvaturelimit,weshowthatthedualhydrodynamicalsystemisdescribedbyageneralizedforcedincompressibleNavier–Stokesequation.Specially,forstationaryblackholesorthosespacetimewithsomeasymptoticallystationaryconditions,suchasystemreducestoastandardforcedNavier–Stokessystem.
Poorman'sholography:howfarcanitgo?
Almostacenturyago,Einstein,afterNewton,shednewlightongravitybyclaimingthatgravityisgeometry.Therehasbeennodeeperinsightbeyondthatlateronexcepttherecentsuspicionthatgravitymayalsobeholographic,dualtosomesortofquantumfieldtheorylivingontheboundarywithonelessdimension.Suchasuspicionhasbeensupportedmainlybyavarietyofspecificexamplesfromstringtheory.Thispaperisintendedtopurporttheholographicgravityfromadifferentperspective.Namely,weshallshowthatsuchaholographycanactuallybeobservedbyworkingmerelywithinthecontextofEinstein'sgravitythroughpromotingBrown–York'sformalism,whereneitheristhespacetimerequiredtobeasymptoticallyAdSnortheboundarytobelocatedatconformalinfinity,whichalsoconformstothespiritinheritedfromWilson'seffectivefieldtheory.Inparticular,weshowthatourholographyworksremarkablywellatleastatthelevelofthermodynamicsandhydrodynamics,whereaperfectmatchingbetweenthebulkgravityandboundaryfluidisfoundforentropyanditsproductionbytheconservedcurrentmethod.
GeometrieswiththeSecondPoincaréSymmetry
ThesecondPoincarékinematicalgroupservesasoneofnewonesinadditiontotheknownpossiblekinematics.ThegeometrieswiththesecondPoincarésymmetryispresentedandtheirpropertiesareanalyzed.Onthegeometries,thenewmechanicsbasedontheprincipleofrelativitywithtwouniversalconstants(c,l)canbeestablished.
IncompressibleNavier–StokesequationfromEinstein–MaxwellandGauss–Bonnet–Maxwelltheories
Thedualfluiddescriptionforageneralcutoffsurfaceatradiusr=rcoutsidethehorizoninthechargedAdSblackbranebulkspace–timeisinvestigated,firstintheEinstein–Maxwelltheory.Underthenon-relativisticlong-wavelengthexpansionwithparameterϵ,thecoupledEinstein–MaxwellequationsaresolveduptoO(ϵ2).TheincompressibleNavier–Stokesequationwithexternalforcedensityisobtainedastheconstraintequationatthecutoffsurface.Fornon-extremalblackbrane,theviscosityofthedualfluidisdeterminedbytheregularityofthemetricfluctuationatthehorizon,whoseratiotoentropydensityη/sisindependentofboththecutoffrcandtheblackbranecharge.Then,weextendourdiscussiontotheGauss–Bonnet–Maxwellcase,wheretheincompressibleNavier–Stokesequationwithexternalforcedensityisalsoobtainedatageneralcutoffsurface.Inthiscase,itturnsoutthattheratioη/sisindependentofthecutoffrcbutdependentonthechargedensityoftheblackbrane.
FromPetrov-EinsteintoNavier–Stokesinspatiallycurvedspacetime
WegeneralizetheframeworkinarXiv:1104.5502tothecasethatanembeddingmayhaveanon-vanishingintrinsiccurvature.DirectlyemployingtheBrown-Yorkstresstensorasthefundamentalvariables,westudytheeffectoffiniteperturbationsoftheextrinsiccurvaturewhilekeepingtheintrinsicmetricfixed.WeshowthatimposingaPetrovtypeIconditiononthehypersurfacegeometrymayreducetotheincompressibleNavier–Stokesequationforafluidmovinginspatiallycurvedspacetimeinthenear-horizonlimit.
Newman-Penroseconstantsofstationaryelectrovacuumspace-times
AtheoremrelatedtotheNewman-Penroseconstantsisproven.ThetheoremstatesthatalltheNewman-Penroseconstantsofasymptoticallyflat,stationary,asymptoticallyalgebraicallyspecialelectrovacuumspace-timesarezero.StraightforwardapplicationofthistheoremshowsthatalltheNewman-PenroseconstantsoftheKerr-Newmanspace-timemustvanish.
UniquenessofKerrspace-timenearnullinfinity
WereexpresstheKerrmetricinstandardBondi-Sachscoordinatesnearnullinfinity
GRAVITATIONALANOMALYANDHAWKINGRADIATIONOFBRANEWORLDBLACKHOLES
Wilczekandhiscollaborators'anomalycancellationapproachisappliedtothe3DSchwarzschild-andBTZ-likebraneworldblackholesinducedbythegeneralizedmetricsintheRandall–Sundrumscenario.Basedonthefactthatthehorizonofbraneworldblackholewillextendintothebulkspacetime,calculationisdonefromthebulkgeneralizedmetricssideanditisshownthatthisapproachalsoreproducesthecorrectHawkingradiationforthesebraneworldblackholes.Besides,sincethisapproachdoesnotinvolvethedynamicalequation,itisalsoshownthattheHawkingradiationisonlyakinematiceffect.
Proofoftheentropyboundondynamicalhorizons
Theentropyboundconjectureconcerningblackholedynamicalhorizonsisproved.Theconjecturestates,ifadynamicalhorizon,DH,isboundedbytwosurfaceswithareasofABandAB'(AB'>AB),thentheentropy,SD,thatcrossesDHmustsatisfySD≤¼(AB'−AB).WeshowthatthisconjectureisimpliedbythegeneralizedBoussobound.Consequently,thegeneralizedsecondlawholdsfordynamicalhorizons.Finally,weshowthatthelightlikeBoussoboundanditsspacelikecounterpartcanbeunifiedasonebound.
OnNewman–Penroseconstantsofstationaryspacetimes
Weconsiderthegeneralasymptoticexpressionofstationaryspacetime.UsingtheKillingequation,wereducethedynamicalfreedomoftheEinsteinequationtothein-goinggravitationalwaveΨ0.Thegeneralformofthisfunctioncanbeobtained.Withthehelpofanasymptoticallyalgebraicspecialcondition,weprovethatallNewman–Penroseconstantsvanish.
Quasilocalenergy-momentumandenergyfluxatnullinfinity
Thenullinfinitylimitofthegravitationalenergy-momentumandenergyfluxdeterminedbythecovariantHamiltonianquasilocalexpressionsisevaluatedusingtheNewman-Penrosespincoefficients.Thereferencecontributionisconsideredbythreedifferentembeddingapproaches.AllofthemgivetheexpectedBondienergyandenergyflux
Diffeomorphisminvarianceandblackholeentropy
TheNoether-chargeandtheHamiltonianrealizationsforthediff(M)algebraindiffeomorphism-invariantgravitationaltheorieswithoutacosmologicalconstantinanydimensionarestudiedinacovariantformalism.