학술논문

Light nuclei collectivity from sNN=3 GeV Au+Au collisions at RHIC
Document Type
article
Author
M.S. AbdallahB.E. AboonaJ. AdamL. AdamczykJ.R. AdamsJ.K. AdkinsG. AgakishievI. AggarwalM.M. AggarwalZ. AhammedA. AitbaevI. AlekseevD.M. AndersonA. AparinE.C. AschenauerM.U. AshrafF.G. AtetallaG.S. AverichevV. BairathiW. BakerJ.G. Ball CapK. BarishA. BeheraR. BellwiedP. BhagatA. BhasinJ. BielcikJ. BielcikovaI.G. BordyuzhinJ.D. BrandenburgA.V. BrandinX.Z. CaiH. CainesM. Calderón de la Barca SánchezD. CebraI. ChakaberiaP. ChaloupkaB.K. ChanF.-H. ChangZ. ChangA. ChatterjeeS. ChattopadhyayD. ChenJ. ChenJ.H. ChenX. ChenZ. ChenJ. ChengS. ChoudhuryW. ChristieX. ChuH.J. CrawfordM. CsanádM. DaugherityT.G. DedovichI.M. DeppnerA.A. DerevschikovA. DhamijaL. Di CarloL. DidenkoP. DixitX. DongJ.L. DrachenbergE. DuckworthJ.C. DunlopJ. EngelageG. EppleyS. EsumiO. EvdokimovA. EwiglebenO. EyserR. FatemiF.M. FawziS. FazioC.J. FengY. FengE. FinchY. FisyakA. FranciscoC. FuC.A. GagliardiT. GalatyukF. GeurtsN. GhimireA. GibsonK. GopalX. GouD. GrosnickA. GuptaW. GurynA. HamedY. HanS. HarabaszM.D. HarastyJ.W. HarrisH. HarrisonS. HeW. HeX.H. HeY. HeS. HeppelmannN. HerrmannE. HoffmanL. HolubC. HuQ. HuY. HuH. HuangH.Z. HuangS.L. HuangT. HuangX. HuangY. HuangT.J. HumanicD. IsenhowerM. IsshikiW.W. JacobsC. JenaA. JentschY. JiJ. JiaK. JiangX. JuE.G. JuddS. KabanaM.L. KabirS. KagamasterD. KalinkinK. KangD. KapukchyanK. KauderH.W. KeD. KeaneA. KechechyanM. KelseyY.V. KhyzhniakD.P. KikołaB. KimelmanD. KincsesI. KiselA. KiselevA.G. KnospeH.S. KoL. KochendaA. KorobitsinL.K. KosarzewskiL. KramarikP. KravtsovL. KumarS. KumarR. Kunnawalkam ElayavalliJ.H. KwasizurR. LaceyS. LanJ.M. LandgrafJ. LauretA. LebedevR. LednickyJ.H. LeeY.H. LeungN. LewisC. LiW. LiX. LiY. LiX. LiangY. LiangR. LicenikT. LinY. LinM.A. LisaF. LiuH. LiuP. LiuT. LiuX. LiuY. LiuZ. LiuT. LjubicicW.J. LlopeR.S. LongacreE. LoydT. LuN.S. LukowX.F. LuoL. MaR. MaY.G. MaN. MagdyD. MallickS.L. ManukhovS. MargetisC. MarkertH.S. MatisJ.A. MazerN.G. MinaevS. MioduszewskiB. MohantyM.M. MondalI. MooneyD.A. MorozovA. MukherjeeM. NagyJ.D. NamMd. NasimK. NayakD. NeffJ.M. NelsonD.B. NemesM. NieG. NigmatkulovT. NiidaR. NishitaniL.V. NogachT. NonakaA.S. NunesG. OdyniecA. OgawaS. OhV.A. OkorokovK. OkuboB.S. PageR. PakJ. PanA. PandavA.K. PandeyY. PanebratsevP. ParfenovA. PaulB. PawlikD. PawlowskaC. PerkinsL.S. PinskyJ. PlutaB.R. PokhrelJ. PorterM. PosikV. ProzorovaN.K. PruthiM. PrzybycienJ. PutschkeH. QiuA. QuinteroC. RaczS.K. RadhakrishnanN. RahaR.L. RayR. ReedH.G. RitterM. RobotkovaO.V. RogachevskiyJ.L. RomeroD. RoyL. RuanA.K. SahooN.R. SahooH. SakoS. SalurE. SamigullinJ. SandweissS. SatoW.B. SchmidkeN. SchmitzB.R. SchweidF. SeckJ. SegerR. SetoP. SeybothN. ShahE. ShahalievP.V. ShanmuganathanM. ShaoT. ShaoR. SharmaA.I. SheikhD.Y. ShenS.S. ShiY. ShiQ.Y. ShouE.P. SichtermannR. SikoraJ. SinghS. SinghaP. SinhaM.J. SkobyN. SmirnovY. SöhngenW. SolystY. SongH.M. SpinkaB. SrivastavaT.D.S. StanislausM. StefaniakD.J. StewartM. StrikhanovB. StringfellowA.A.P. SuaideM. SumberaB. SummaX.M. SunX. SunY. SunB. SurrowD.N. SviridaZ.W. SwegerP. SzymanskiA.H. TangZ. TangA. TaranenkoT. TarnowskyJ.H. ThomasA.R. TimminsD. TlustyT. TodorokiM. TokarevC.A. TomkielS. TrentalangeR.E. TribbleP. TribedyS.K. TripathyT. TruhlarB.A. TrzeciakO.D. TsaiZ. TuT. UllrichD.G. UnderwoodI. UpsalG. Van BurenJ. VanekA.N. VasilievI. VassilievV. VerkestF. VidebækS. VokalS.A. VoloshinF. WangG. WangJ.S. WangP. WangX. WangY. WangZ. WangJ.C. WebbP.C. WeidenkaffG.D. WestfallH. WiemanS.W. WissinkR. WittJ. WuY. WuB. XiZ.G. XiaoG. XieW. XieH. XuN. XuQ.H. XuY. XuZ. XuG. YanC. YangQ. YangS. YangY. YangZ. YeL. YiK. YipY. YuH. ZbroszczykW. ZhaC. ZhangD. ZhangJ. ZhangS. ZhangY. ZhangZ.J. ZhangZ. ZhangF. ZhaoJ. ZhaoM. ZhaoC. ZhouY. ZhouX. ZhuM. ZurekM. Zyzak
Source
Physics Letters B, Vol 827, Iss , Pp 136941- (2022)
Subject
Physics
QC1-999
Language
English
ISSN
0370-2693
Abstract
In high-energy heavy-ion collisions, partonic collectivity is evidenced by the constituent quark number scaling of elliptic flow anisotropy for identified hadrons. A breaking of this scaling and dominance of baryonic interactions is found for identified hadron collective flow measurements in sNN = 3 GeV Au+Au collisions. In this paper, we report measurements of the first- and second-order azimuthal anisotropic parameters, v1 and v2, of light nuclei (d, t, 3He, 4He) produced in sNN = 3 GeV Au+Au collisions at the STAR experiment. An atomic mass number scaling is found in the measured v1 slopes of light nuclei at mid-rapidity. For the measured v2 magnitude, a strong rapidity dependence is observed. Unlike v2 at higher collision energies, the v2 values at mid-rapidity for all light nuclei are negative and no scaling is observed with the atomic mass number. Calculations by the Jet AA Microscopic Transport Model (JAM), with baryonic mean-field plus nucleon coalescence, are in good agreement with our observations, implying baryonic interactions dominate the collective dynamics in 3 GeV Au+Au collisions at RHIC.