Large N gauge theories -- Numerical results
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Some physical results in four dimensional large N gauge theories on a periodic torus are summarized.
February1,200823:52WSPC-ProceedingsTrimSize:9inx6intalk
6
002 luJ 02 1v941706/0ht-pe:hviXra1
LargeNgaugetheories–Numericalresults
R.Narayanan
DepartmentofPhysics,FloridaInternationalUniversity,
Miami,FL33199,USA
E-mail:rajamani.narayanan@ u.edu
H.Neuberger
RutgersUniversity,DepartmentofPhysicsandAstronomy,
Piscataway,NJ08855,USA
E-mail:neuberg@physics.rutgers.edu
SomephysicalresultsinfourdimensionallargeNgaugetheoriesonaperiodictorusaresummarized.
Keywords:LargeNQCD,decon nement,phasetransitions.
1.Introduction
tticeQCDisausefultechniqueforextractingfundamentalresultsinthelargeNlimitofQCD.Fermionsarenaturallyquenchedinthe’tHooftlimitoflargeNQCDandthissigni cantlyreducesthecomputationalcostinalatticecalculation.Inaddition,thereisaconceptofcontinuumreduction3,namely,physicsdoesnotdependonthesizeofboxl4forl>lcandlcisaphysicalcriticalsize.ThesetwoobservationshavebeenusedtoextractphysicalresultsinthelargeNlimitofQCDusingnumericaltechniquesonthelattice.
2.PhasesoflargeNQCD
LargeNQCDonacontinuumtorusl4hasseveralphases4dependinguponthesizeofthetorusasshowninFig.1.ThecontinuumactionhasU4(1)symmetriesassociatedwiththePolyakovloopsinthefourdirectionsandthevariousphasescorrespondtothenumberofdirectionsinwhichthis
Some physical results in four dimensional large N gauge theories on a periodic torus are summarized.
2
symmetryisbroken.Thecontinuumlimitisobtainedbygoingtothetop-rightcornerofFig.1anddi erentapproachestothiscornerwillresultinoneofthe vecontinuumphases.
The0h-phasepresentforb<0.36forallLisanunphysicalphasethatdoesnotsurvivethecontinuumlimit.The0hto0ctransitionisassoci-atedwiththesingleplaquetteoperatoropeningupagaparoundπinitseigenvaluedistribution.Gauge eldscomeindisconnectedpiecesinalltheXc-phasesduetothepresenceofthegapinthesingleplaquetteoperator5.
The0c-phaseisthecon nedphaseoflargeNQCDandthe1c-phaseisthedecon nedphaseandlc=1/tc.Animmediateconsequenceofcon-tinuumreductionisthatlargeNQCDdoesnotfeeltemperaturesbelowtc6.Numericalanalysishasshownthatlatticespacinge ectsaresmallinthe0c-phaseanditissu cienttoworkatL~9andN~30toextractcontinuumresults.Therefore,numericalcomputationscanbeperformedonaserialcomputerandaclusterofcomputerscanbee cientlyusedtogeneratestatisticsinaMonte-Carlocalculation.
Some physical results in four dimensional large N gauge theories on a periodic torus are summarized.
3
tticecoupling.
3.Chiralsymmetrybreakingin nitevolume
Sincephysicsdoesnotdependontheboxsizein0c-phase,oneshouldshowthatchiralsymmetryisspontaneouslybrokenin nitevolumeinordertoproperlyreproducephysicsinthisphase7.Theorderoflimitsareimpor-tantandonehastotakethelargeNlimitbeforetakingthequarkmasstozeroat nitephsyicalvolume.ThelowlyingspectrumofthemasslessDiracoperatorshowsevidenceforspontaneouschiralbreakingsincetheeigenval-ues,iλ,scaleslikez=λΣNl4withzobeyingauniversaldistribution.Thechiralcondesate,Σ,isindependentofl.ResultsofacalculationofthechiralcondensateonthelatticeisshowninFig.2.Resultsfromchiralrandommatrixtheory8wereusedtoextractthechiralcondensateata xedN,Landlatticecoupling.Twolowestnon-zeroeigenvaluesintheQ=0andQ=1topologicalsectorswereusedtoshowconsistency.TheplotshowsthatthereisalimitasN→∞andthislimitisindependentofL.Results
obtainedatdi erentlatticecouplingsyieldl3
c
Some physical results in four dimensional large N gauge theories on a periodic torus are summarized.
4
4.PionsinlargeNQCD
SincechiralsymmetryisbrokeninlargeNQCDevenin nitevolume,oneshouldbeabletoobservemasslesspionsin nitevolume.Thisresultemergesinthefollowingmanner9.Propertiesofasinglequarkinaback-groundgauge eldAµ(x)cannotdependonashiftofAµ(x)→Aµ(x)+p
µ
otherseesAµ(x)→Aµ(x)
pµ
2l
andthe
Some physical results in four dimensional large N gauge theories on a periodic torus are summarized.
5
curveasshownin g.3andfπlc=
12Λπ
≈0.269.
5.Chiralsymmetryrestoration
The0cto1cphasetransitionisthecon nement-decon nementphasetransitionsincetheU(1)symmetryassociatedwithoneofthePolyakovloopsisbroken.Thistransitionis rstordersincethereisalatentheatas-sociatedwiththesingleplaquette11.Thefermiondeterminantdoesmatterinthe1c-phaseanditpicksthecorrectboundaryconditionsforfermionsinthebrokendirection,namely,anti-periodicwithrespecttothePolyakovloop12.ThelowesteigenvalueoftheDiracoperatorwiththecorrectbound-aryconditionscanbeusedtostudythegapinthe1c-phaseandone ndsthatchiralsymmetryisrestoredinthe1c-phase12.Furthermore,thechiraltransitionis rstorderasshowninFig.4.Ifoneweretosuper-coolthe1c-phaseintothe0c-phase,asecondordertransitionwithasquarerootsingularitywouldbeobservedat0.93/lc.
Some physical results in four dimensional large N gauge theories on a periodic torus are summarized.
6
6.PhasetransitionintheWilsonloopoperator
Non-abeliangaugetheoriesinthecon nedphasearestronglyinteractingatlargedistancesandweaklyinteractingatshortdistances.Ifthisisseenasaphasetransitioninsomeobservable,onecouldusetheuniversalbehaviorofthistransitiontoconnectthelowenergyphysicsofQCDtothehighenergyphysicsofQCD.TheWilsonloopoperatorasafunctionofitssizeisthemostlikelycandidatetostudythistransitionwithinthe0c-phaseoflargeNQCD13.SuchatransitionexistsintwodimensionallargeNQCD14anditisclaimedthatthetransitioninfourdimensionalQCDisinthesameuniversalityclass.ThistransitionisreferredtoastheDurhuus-OlesenphasetransitioninFig1.
asafunctionofitssizeinlargeNQCD.ThedistributionoftheeigenvaluesofthesmearedWilsonloopoperatorarecomparedtotheDurhuus-Olesendistributions.Re-sultsareshownforloopsofsizesl/lc=0.740,0.660,0.560,0.503.Theymatchwithk=4.03,2.30,1.41,1.15wherekisthedimensionlessareaintwodimensionlargeNQCD.k=2isthecriticalarea.
Wilsonloopoperatorssu erfromaperimeterdivergenceinfourdimen-sionsandonehastoeliminateitwhende ningthisoperatorifonewereto
Some physical results in four dimensional large N gauge theories on a periodic torus are summarized.
7
studyitseigenvaluedistribution.Onepossiblewaytosuppresstheperime-terdivergenceistousesmearedoperatorsonthelattice.NumericalstudiesoftheeigenvaluedistributionofthesmearedWilsonloopoperatoronthelatticeshowsclearevidenceforaphasetransitionasafunctionofthesizeoftheWilsonloop13.TheuniversalityclassisthesameastheonefoundintwodimensionallargeNQCDasshowninFig.5andthecriticalloopsizeisroughly0.6lc.Acknowledgements
R.N.wouldliketothanktheorganizersofCAQCD-06forastimulat-ingatmosphere.R.N.acknowledgespartialsupportbytheNSFundergrantnumberPHY-0300065andpartialsupportfromJe ersonLab.TheThomasJe ersonNationalAcceleratorFacility(Je ersonLab)isoperatedbytheSoutheasternUniversitiesResearchAssociation(SURA)underDOEcontractDE-AC05-84ER40150.H.N.acknowledgespartialsupportbytheDOEundergrantnumberDE-FG02-01ER41165atRutgersUniversity.References
1.A.V.Manohar,arXiv:hep-ph/9802419.
2.O.Aharony,S.S.Gubser,J.M.Maldacena,H.OoguriandY.Oz,Phys.Rept.323,183(2000)[arXiv:hep-th/9905111].
3.J.Kiskis,R.NarayananandH.Neuberger,“Doesthecrossoverfromper-turbativetononperturbativephysicsinQCDPhys.Lett.B574,65(2003)[arXiv:hep-lat/0308033].
4.R.NarayananandH.Neuberger,PoSLAT2005,005(2006)[arXiv:hep-lat/0509014].
5.J.Kiskis,R.NarayananandH.Neuberger,Phys.Rev.D66,025019(2002)[arXiv:hep-lat/0203005].
6.T.D.Cohen,Phys.Rev.Lett.93,201601(2004)[arXiv:hep-ph/0407306].7.R.NarayananandH.Neuberger,Nucl.Phys.B696,107(2004)[arXiv:hep-lat/0405025].
8.J.J.M.VerbaarschotandT.Wettig,Ann.Rev.Nucl.Part.Sci.50,343(2000)[arXiv:hep-ph/0003017].
9.R.NarayananandH.Neuberger,Phys.Lett.B616,76(2005)[arXiv:hep-lat/0503033].
10.D.J.GrossandY.Kitazawa,Nucl.Phys.B206,440(1982).11.J.Kiskis,arXiv:hep-lat/0507003.
12.R.NarayananandH.Neuberger,Phys.Lett.B638,546(2006)[arXiv:hep-th/0605173].
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