6533b830fe1ef96bd12979de
RESEARCH PRODUCT
Neutral pion production with respect to centrality and reaction plane in Au+Au collisions atsNN=200GeV
K. KaratsuY. NakamiyaJ. P. WoodAnne Marie SicklesG. BaksayAlexander MilovC. M. CamachoPrashant ShuklaI. NakagawaR. LuechtenborgTaku GunjiH. GongS. F. PateB. KomkovT. EngelmoreJ. SeeleY. TanakaF. KajiharaM. OuchidaE. MannelO. DrapierN. MeansFrank EllinghausB. SahlmuellerB. SahlmuellerNorio SaitoH. Al-batainehG. R. YoungE. R. KinneyM. A. L. LeiteY. J. KimD. P. MorrisonE. J. DesmondS. ButsykS. CampbellS. ZhouM. TogawaE. Vazquez-zambranoY. FukaoJ. ParkT. HesterL. BaksayV. PapavassiliouTatsuya ChujoN. A. SparksC. L. WoodyA. BerdnikovT. IchiharaS. D. RolnickA. RakotozafindrabeN. GrauN. GrauY. OnukiMotoi InabaR. M. WrightTadaaki IsobeJen-chieh PengR. BelmontJ. S. KapustinskyV. BabintsevAlice MignereyJan RakR. LaceyY. TsuchimotoMate CsanadV. S. PantuevK. N. BarishP. L. McgaugheyR. A. SoltzTakao SakaguchiK. A. DreesCharles MaguireInkyu ParkF. MatathiasKensuke HommaE. RichardsonG. S. KyleR. Granier De CassagnacA. AdareTakahiro FusayasuS. BatheS. BatheI. E. YushmanovS. TarafdarAjit Kumar MohantyT. A. ShibataR. P. PisaniT. SatoXiong WangAgneta OskarssonJ. HamblenS. SanoS. SanoJames AlexanderI. V. SourikovaM. Grosse PerdekampR. PakVladimir SamsonovE. KistenevN. KamiharaA. D. FrawleyP. ConstantinK. WatanabeR. AverbeckByung-sik HongDong Jo KimR. VértesiR. VértesiA. BazilevskyM. KurosawaSung Keun ParkM. E. ConnorsD. IsenhowerA. ToiaT. L. ThomasTakafumi NiidaAlexander MalakhovB. BassalleckS. HuangK. S. SimK. OkadaTamas Ferenc CsorgoR. YangK. ShojiA. V. KazantsevPhilippe RosnetW. HolzmannMaya Hachiya ShimomuraM. L. BrooksAlexandre LebedevJ. L. NagleH. PeiM. KonnoN. N. AjitanandK. TanidaJ. E. FrantzJ. E. FrantzL. TomášekP. MikešP. MikešH. En'yoA. VeichtM. J. LeitchK. ImaiK. ImaiShinhong KimD. M. LeeRyugo S. HayanoEva HaslumY. RiabovKenta ShigakiY. I. MakdisiM. NguyenD. SilvermyrL. S. ZolinPeter ChristiansenA. S. NyaninD. WinterY. BerdnikovY. AkibaM. I. NagyM. MishraD. WatanabeS. NagamiyaM. D. MalikE. VznuzdaevK. KirilukA. DreesW. J. ParkChristopher RosenX. HeB. LenziI. TserruyaT. HoraguchiP. W. StankusS. AfanasievYu. EfremenkoRachid NouicerE. H. KimM. ProisslD. Yu PeressounkoH. A. GustafssonP. TarjánTakahiro NakamuraB. AzmounA. KrálP. ChungM. WysockiY. J. KwonA. YanovichJ. T. MitchellMarisilvia DonadelliV. BumazhnovY. AramakiM. J. TannenbaumV. PeresedovAlexei KhanzadeevV. SinghH. ToriiT. C. AwesE. StenlundKyoichiro OzawaT. LiškaR. TanabeJongmin LeeJ. JinC. ZhangVaclav VrbaKlaus Johannes ReygersRui WeiJ. NewbyA. DattaJ. S. BokR. SeidlVladislav MankoP. RužičkaSusumu OdaA. DurumJ. KosterE. M. TakaguiM. SlunečkaR. S. TowellM. ChiuD. KotchetkovI. GarishviliB. MeredithA. DeshpandeViktor RiabovRushan HanF. WeiH. MasuiK. DasCatherine Micaela SilvestreS. BelikovK. YamauraD. HornbackC. A. OgilvieKisung LeeT. K. HemmickJohn HillKyeongpil LeeSenta GreeneA. A. BickleyM. OkaBeomkyu KimK. BoyleWei XieA. T. BasyeEunja KimJ. M. DurhamYasuo MiakeToru SugitateE. P. HartouniC. ValeC. ValeJ. IdeW. A. ZajcB. LoveT. V. MoukhanovaHongfang LiuHongfang LiuD. E. FieldsB. V. JacakB. FademE. O'brienV. BaublisH. QuA. KissA. DenisovV. CiancioloA. DionL. KochendaM. IssahA. G. LitvinenkoS. SawadaM. MccumberA. TaranenkoHideki HamagakiK. AokiKazushi MikiC. Y. ChiSergey FokinA. KozlovBrajesh K. SinghD. LynchJ. HanksHenner BueschingSteve EdwardsK. SakashitaFrançois FleuretR. SetoG. DavidJ. YingA. FranzK. I. HahnC. BaumannS. KametaniI. DanchevA. EnokizonoP. LiebingS. N. WhiteJason KaminC. P. SinghS. P. StollZvi Hirsh CitronS. S.e. RosendahlG. BunceK. S. JooB. M. JohnsonK. NakanoD. JouanW. E. SondheimMarcus HohlmannD. IvanischevA. IsupovA. TaketaniL. A. Linden LevyY. WatanabeD. S. JumperT. KempelJ. SziklaiP. A. RukoyatkinA. K. PurwarK. FujiwaraS. EsumiY. L. YamaguchiD. SharmaR. IchimiyaDong-hun KimE. LeitnerBrian ColeI. YounusI. YounusMartin PurschkeC. A. AidalaC. A. AidalaH. W. Van HeckeA. MorrealeZ. FraenkelR. K. ChoudhuryT. DahmsM. NaglisC. L. SilvaI. RavinovichMasayasu IshiharaD. KawallH. ThemannJ. MurataGerd Joachim KundeI. SheinM. BaiK. SedgwickZhiying YouR. BennettM. KawashimaM. FingerS. DairakuM. ViriusC. H. ChenA. GlennM. RosatiA. A. VinogradovJiangyong JiaJiangyong JiaY. GotoO. DietzschE. T. AtomssaH. ValleDipanwita DuttaJulia VelkovskaK. B. LeeD. RoachK. M. KijimaXingguo LiS. P. SorensenO. ChvalaJ. G. LajoieI. J. ChoiA. KravitzM. GoninA. SukhanovK. KuritaH. PereiraY. MorinoY. J. MaoJ. H. KangJ. S. HaggertyJohannes Peter WesselsY. S. LaiY. IkedaC. PinkenburgMinghui LiuM. HeffnerKenneth Francis ReadKenneth Francis ReadG. RocheA. Yu. SemenovS. Yokkaichisubject
PhysicsQuantum chromodynamicsNuclear physicsNuclear and High Energy PhysicsAdS/CFT correspondenceParticle physicsPionLuminosity (scattering theory)Path lengthConformal field theoryPartonRelativistic Heavy Ion Colliderdescription
The PHENIX experiment has measured the production of pi(0)s in Au + Au collisions at root S-NN = 200 GeV. The new data offer a fourfold increase in recorded luminosity, providing higher precision and a larger reach in transverse momentum, p(T), to 20 GeV/c. The production ratio of eta/pi(0) is 0.46 +/- 0.01(stat) +/- 0.05(syst), constant with p(T) and collision centrality. The observed ratio is consistent with earlier measurements, as well as with the p + p and d + Au values. pi(0) are suppressed by a factor of 5, as in earlier findings. However, with the improved statistical precision a small but significant rise of the nuclear modification factor R-AA vs p(T), with a slope of 0.0106 +/-(0.0034)(0.0029) (Gev/c)(-1), is discernible in central collisions. A phenomenological extraction of the average fractional parton energy loss shows a decrease with increasing p(T). To study the path-length dependence of suppression, the pi(0) yield is measured at different angles with respect to the event plane; a strong azimuthal dependence of the pi(0) R-AA is observed. The data are compared to theoretical models of parton energy loss as a function of the path length L in the medium. Models based on perturbative quantum chromodynamics are insufficient to describe the data, while a hybrid model utilizing pQCD for the hard interactions and anti-de-Sitter space/conformal field theory (AdS/CFT) for the soft interactions is consistent with the data. DOI: 10.1103/PhysRevC.87.034911
year | journal | country | edition | language |
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2013-03-28 | Physical Review C |