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2022-01-25
Collision-System and Beam-Energy Dependence of Anisotropic Flow Fluctuations
STAR CollaborationM. S. AbdallahJ. AdamL. AdamczykJ. R. AdamsJ. K. AdkinsG. AgakishievI. AggarwalM. M. AggarwalZ. AhammedI. AlekseevD. M. AndersonA. AparinE. C. AschenauerM. U. AshrafF. G. AtetallaA. AttriG. S. AverichevV. BairathiW. BakerJ. G. Ball CapK. BarishA. BeheraR. BellwiedP. BhagatA. BhasinJ. BielcikJ. BielcikovaI. G. BordyuzhinJ. D. BrandenburgA. V. BrandinI. BunzarovJ. ButterworthX. Z. CaiH. CainesM. Calderón de la Barca SánchezD. CebraI. ChakaberiaP. ChaloupkaB. K. ChanF-H. ChangZ. ChangN. Chankova-BunzarovaA. ChatterjeeS. ChattopadhyayD. ChenJ. ChenJ. H. ChenX. ChenZ. ChenJ. ChengM. ChevalierS. ChoudhuryW. ChristieX. ChuH. J. CrawfordM. CsanádM. DaugherityT. G. DedovichI. M. DeppnerA. A. DerevschikovA. DhamijaL. Di CarloL. DidenkoP. DixitX. DongJ. L. DrachenbergE. DuckworthJ. C. DunlopN. ElseyJ. EngelageG. EppleyS. EsumiO. EvdokimovA. EwiglebenO. EyserR. FatemiF. M. FawziS. FazioP. FedericJ. FedorisinC. J. FengY. FengP. FilipE. FinchY. FisyakA. FranciscoC. FuL. FulekC. A. GagliardiT. GalatyukF. GeurtsN. GhimireA. GibsonK. GopalX. GouD. GrosnickA. GuptaW. GurynA. I. HamadA. HamedY. HanS. HarabaszM. D. HarastyJ. W. HarrisH. HarrisonS. HeW. HeX. H. HeY. HeS. HeppelmannS. HeppelmannN. HerrmannE. HoffmanL. HolubY. HuH. HuangH. Z. HuangS. L. HuangT. HuangX. HuangY. HuangT. J. HumanicG. IgoD. IsenhowerW. 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. KikołaC. KimB. KimelmanD. KincsesI. KiselA. KiselevA. G. KnospeL. KochendaL. K. KosarzewskiL. KramarikP. KravtsovL. KumarS. KumarR. Kunnawalkam ElayavalliJ. H. KwasizurR. LaceyS. LanJ. M. LandgrafJ. LauretA. LebedevR. LednickyJ. H. LeeY. H. LeungC. LiC. LiW. LiX. LiY. LiX. LiangY. LiangR. LicenikT. LinY. LinM. A. LisaF. LiuH. LiuH. LiuP. LiuT. LiuX. LiuY. LiuZ. LiuT. LjubicicW. J. LlopeR. S. LongacreE. LoydN. S. LukowX. F. LuoL. MaR. MaY. G. MaN. MagdyD. MallickS. 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. OkorokovB. S. PageR. PakA. PandavA. K. PandeyY. PanebratsevP. ParfenovB. PawlikD. PawlowskaH. PeiC. PerkinsL. PinskyR. L. PintérJ. PlutaB. R. PokhrelG. PonimatkinJ. PorterM. PosikV. ProzorovaN. K. PruthiM. PrzybycienJ. PutschkeH. QiuA. QuinteroC. RaczS. K. RadhakrishnanN. RahaR. L. RayR. ReedH. G. RitterM. RobotkovaO. V. RogachevskiyJ. L. RomeroD. RoyL. RuanJ. RusnakN. R. SahooH. SakoS. SalurJ. SandweissS. SatoW. B. SchmidkeN. SchmitzB. R. SchweidF. SeckJ. SegerM. SergeevaR. SetoP. SeybothN. ShahE. ShahalievP. V. ShanmuganathanM. ShaoT. ShaoA. I. SheikhD. ShenS. S. ShiY. ShiQ. Y. ShouE. P. SichtermannR. SikoraM. SimkoJ. SinghS. SinghaM. J. SkobyN. SmirnovY. SöhngenW. SolystP. SorensenH. M. SpinkaB. SrivastavaT. D. S. StanislausM. StefaniakD. J. StewartM. StrikhanovB. StringfellowA. A. P. SuaideM. SumberaB. SummaX. M. SunX. SunY. 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. VoloshinG. WangJ. S. WangP. WangY. WangY. WangZ. WangJ. C. WebbP. C. WeidenkaffL. WenG. D. WestfallH. WiemanS. W. WissinkJ. WuY. WuB. XiZ. G. XiaoG. XieW. XieH. XuN. XuQ. H. XuY. XuZ. XuZ. XuC. YangQ. YangS. YangY. YangZ. YeZ. YeL. YiK. YipY. YuH. ZbroszczykW. ZhaC. ZhangD. ZhangJ. ZhangS. ZhangS. ZhangX. P. ZhangY. ZhangY. ZhangY. ZhangZ. J. ZhangZ. ZhangZ. ZhangJ. ZhaoC. ZhouX. ZhuZ. ZhuM. ZurekM. Zyzak
文献摘要
Elliptic flow measurements from two-, four- and six-particle correlations are used to investigate flow fluctuations in collisions of U+U at $\sqrt{s_{\rm NN}}\sqrt{s_{\rm NN}}$= 200 GeV and Au+Au spanning the range = 11.5 - 200 GeV. The measurements show a strong dependence of the flow fluctuations on collision centrality, a modest dependence on system size, and very little if any, dependence on particle species and beam energy. The results, when compared to similar LHC measurements, viscous hydrodynamic calculations, and TENTo model eccentricities, indicate that initial-state-driven fluctuations predominate the flow fluctuations generated in the collisions studied.
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