Elliptic flow of identified hadrons in Au+Au collisions at sNN=\sqrt{s_{NN}}= 7.7--62.4 GeV

preprint2013arXivOpen access
L. AdamczykJ. K. AdkinsG. AgakishievM. M. AggarwalZ. AhammedI. AlekseevJ. AlfordC. D. AnsonA. AparinD. ArkhipkinE. AschenauerG. S. AverichevJ. BalewskiA. BanerjeeZ. BarnovskaD. R. BeavisR. BellwiedM. J. BetancourtR. R. BettsA. BhasinA. K. BhatiBhattaraiH. BichselJ. BielcikJ. BielcikovaL. C. BlandI. G. BordyuzhinW. BorowskiJ. BouchetA. V. BrandinS. G. BrovkoE. BrunaS. BültmannI. BunzarovT. P. BurtonJ. ButterworthH. CainesM. Calderón de la Barca SánchezD. CebraR. CendejasM. C. CervantesP. ChaloupkaZ. ChangS. ChattopadhyayH. F. ChenJ. H. ChenJ. Y. ChenL. ChenJ. ChengM. CherneyA. ChikanianW. ChristieP. ChungJ. ChwastowskiM. J. M. CodringtonR. CorlissJ. G. CramerH. J. CrawfordX. CuiS. DasA. Davila LeyvaL. C. De SilvaR. R. DebbeT. G. DedovichJ. DengR. Derradi de SouzaS. DhamijaB. Di RuzzaL. DidenkoDilksF. DingA. DionP. DjawothoX. DongJ. L. DrachenbergJ. E. DraperC. M. DuL. E. DunkelbergerJ. C. DunlopL. G. EfimovM. ElnimrJ. EngelageK. S. EngleG. EppleyL. EunO. EvdokimovR. FatemiS. FazioJ. FedorisinR. G. FerschP. FilipE. FinchY. FisyakC. E. FloresC. A. GagliardiD. R. GangadharanD. GarandF. GeurtsA. GibsonS. GliskeO. G. GrebenyukD. GrosnickY. GuoA. GuptaS. GuptaW. GurynB. HaagO. HajkovaA. HamedL-X. HanR. HaqueJ. W. HarrisJ. P. Hays-WehleS. HeppelmannA. HirschG. W. HoffmannD. J. HofmanS. HorvatB. HuangH. Z. HuangP. HuckT. J. HumanicG. IgoW. W. JacobsC. JenaE. G. JuddS. KabanaK. KangK. KauderH. W. KeD. KeaneA. KechechyanA. KesichD. P. KikolaJ. KirylukI. KiselA. KisielD. D. KoetkeT. KolleggerJ. KonzerI. KoraltW. KorschL. KotchendaP. KravtsovK. KruegerI. KulakovL. KumarM. A. C. LamontJ. M. LandgrafK. D. LandryS. LaPointeJ. LauretA. LebedevR. LednickyJ. H. LeeW. LeightM. J. LeVineC. LiW. LiX. LiY. LiZ. M. LiL. M. LimaM. A. LisaF. LiuT. LjubicicW. J. LlopeR. S. LongacreX. LuoA. LuszczakG. L. MaY. G. MaD. M. M. D. Madagodagettige DonD. P. MahapatraR. MajkaS. MargetisC. MarkertH. MasuiH. S. MatisD. McDonaldT. S. McShaneS. MioduszewskiM. K. MitrovskiY. MohammedB. MohantyM. M. MondalM. G. MunhozM. K. MustafaM. NaglisB. K. NandiMd. NasimT. K. NayakJ. M. NelsonL. V. NogachJ. NovakG. OdyniecA. OgawaK. OhA. OhlsonV. OkorokovE. W. OldagR. A. N. OliveiraD. OlsonM. PachrB. S. PageS. K. PalY. X. PanY. PanditY. PanebratsevT. PawlakB. PawlikH. PeiC. PerkinsW. PerytP. PileM. PlaninicJ. PlutaD. PlykuN. PoljakJ. PorterA. M. PoskanzerC. B. PowellC. PruneauN. K. PruthiM. PrzybycienP. R. PujahariJ. PutschkeH. QiuS. RamachandranR. RaniwalaS. RaniwalaR. L. RayC. K. RileyH. G. RitterJ. B. RobertsO. V. RogachevskiyJ. L. RomeroJ. F. RossA. RoyL. RuanJ. RusnakN. R. SahooP. K. SahuI. SakrejdaS. SalurA. SandaczJ. SandweissE. SangalineA. SarkarJ. SchambachR. P. ScharenbergA. M. SchmahB. SchmidkeN. SchmitzT. R. SchusterJ. SegerP. SeybothN. ShahE. ShahalievM. ShaoB. SharmaM. SharmaW. Q. ShenS. S. ShiQ. Y. ShouE. P. SichtermannR. N. SingarajuM. J. SkobyD. SmirnovN. SmirnovD. SolankiP. SorensenU. G. deSouzaH. M. SpinkaB. SrivastavaT. D. S. StanislausJ. R. StevensR. StockM. StrikhanovB. StringfellowA. A. P. SuaideM. C. SuarezM. SumberaX. M. SunY. SunZ. SunB. SurrowD. N. SviridaT. J. M. SymonsA. Szanto de ToledoJ. TakahashiA. H. TangZ. TangL. H. TariniT. TarnowskyJ. H. ThomasA. R. TimminsD. TlustyM. TokarevS. TrentalangeR. E. TribbleP. TribedyB. A. TrzeciakO. D. TsaiJ. TurnauT. UllrichD. G. UnderwoodG. Van BurenG. van NieuwenhuizenJ. A. Vanfossen, Jr.R. VarmaG. M. S. VasconcelosR. VertesiF. VidebækY. P. ViyogiS. VokalS. A. VoloshinA. VossenM. WadaM. WalkerF. WangG. WangH. WangJ. S. WangQ. WangX. L. WangY. WangG. WebbJ. C. WebbG. D. WestfallH. WiemanS. W. WissinkR. WittY. F. WuZ. XiaoW. XieK. XinH. XuN. XuQ. H. XuW. XuY. XuZ. XuYanC. YangY. YangP. YepesL. YiK. YipI-K. YooY. ZawiszaH. ZbroszczykW. ZhaJ. B. ZhangS. ZhangX. P. ZhangY. ZhangZ. P. ZhangF. ZhaoJ. ZhaoC. ZhongX. ZhuY. H. ZhuY. ZoulkarneevaM. Zyzak

Abstract

Measurements of the elliptic flow, v2v_{2}, of identified hadrons (π±π^{\pm}, K±K^{\pm}, Ks0K_{s}^{0}, pp, pˉ\bar{p}, ϕϕ, ΛΛ, Λˉ\barΛ, Ξ−Ξ^{-}, Ξˉ+\barΞ^{+}, Ω−Ω^{-}, Ωˉ+\barΩ^{+}) in Au+Au collisions at sNN=\sqrt{s_{NN}}= 7.7, 11.5, 19.6, 27, 39 and 62.4 GeV are presented. The measurements were done at mid-rapidity using the Time Projection Chamber and the Time-of-Flight detectors of the STAR experiment during the Beam Energy Scan program at RHIC. A significant difference in the v2v_{2} values for particles and the corresponding anti-particles was observed at all transverse momenta for the first time. The difference increases with decreasing center-of-mass energy, sNN\sqrt{s_{NN}} (or increasing baryon chemical potential, μBμ_{B}) and is larger for the baryons as compared to the mesons. This implies that particles and anti-particles are no longer consistent with the universal number-of-constituent quark (NCQ) scaling of v2v_{2} that was observed at sNN=\sqrt{s_{NN}}= 200 GeV. However, for the group of particles NCQ scaling at (mT−m0)/nq>(m_{T}-m_{0})/n_{q}> 0.4 GeV/c2c^{2} is not violated within ±\pm10%. The v2v_{2} values for ϕϕ mesons at 7.7 and 11.5 GeV are approximately two standard deviations from the trend defined by the other hadrons at the highest measured pTp_{T} values.

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