0909.2865v2 d3-d7 quark-gluon plasmas

0909.2865v2 d3-d7 quark-gluon plasmas

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时间:2018-07-28

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1、KUL-TF-09/17D3-D7Quark-GluonPlasmasFrancescoBigazzia,AldoL.Cotroneb,JavierMasc,AngelParedesd,AlfonsoV.Ramalloc,JavierTarr´ıoc.aPhysiqueTh´eoriqueetMath´ematiqueandInternationalSolvayInstitutes,Universit´eLibredeBruxelles;CP231,B-1050Bruxelles,Belgium.bInstitutefortheor

2、eticalphysics,K.U.Leuven;Celestijnenlaan200D,B-3001Leuven,Belgium.cDepartamentodeF´ısicadePart´ıculas,UniversidadedeSantiagodeCompostelaandInstitutoGalegodeF´ısicadeAltasEnerx´ıas(IGFAE);E-15782,SantiagodeCompostela,Spain.dDepartamentdeF´ısicaFonamentalandICCUBInstitut

3、deCi`enciesdelCosmos,UniversitatdeBarcelona,Mart´ıiFranqu`es,1,E-08028,Barcelona,Spain.fbigazzi@ulb.ac.be,cotrone@itf.fys.kuleuven.be,javier.mas@usc.es,aparedes@ffn.ub.es,alfonso@fpaxp1.usc.es,tarrio@fpaxp1.usc.esAbstractWepresentthestringdualtofinitetemperatureSU(Nc)N=4

4、SYMcoupledtomasslessfunda-mentalmatterintroducedbyNfD7branes,withAbelianflavorsymmetry.TheanalyticsolutionarXiv:0909.2865v2[hep-th]7Oct2009includesthebackreactionoftheflavorsuptosecondorderintheparameterthatweighstheinter-nalflavorloops,ǫh=(λhNf)/(8π2Nc),λhbeingthe’tHooft

5、couplingatthetemperatureofthedualQuark-GluonPlasma.Westudythethermodynamicsofthesystemanditsdeparturefromconformality,whichisasecondordereffect.Wethenanalyzetheenergylossofpartonsmovingthroughtheplasma,findingthatthefundamentaldegreesoffreedomenhancethejetquenching.Thewh

6、olesetupisgeneralizedtoD3-D7systemswithD3-branesplacedatthetipofagenericsingularCalabi-Yauconeoverafive-dimensionalSasaki-Einsteinmanifold.WefinallyprovidetheequationsfortheinclusionofmassiveflavorsintheN=4SYMplasma.11IntroductionThe“fireballs”experimentallyproducedatRHICa

7、ndtheonesthatwillbeproducedattheLHCcontainanon-zerofractionofdegreesoffreedominthefundamentalrepresentation[1]:theyaretrulyQuark-GluonPlasmasratherthanjustGluonPlasmas.Whileholographicmethodsprovideinterestingtoolstoanalyzethesesystems,theyhavemainlybeenconcernedwithpl

8、asmaswithoutflavorsinfundamentalrepresentations,orhavetreatedthelatterinthequenchedapproximation.1Thesimplestandbestst

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