Measurement of cold nuclear matter effects for inclusive J/ψJ/ψ in pp+Au collisions at sNN\sqrt{s_{_{\mathrm{NN}}}} = 200 GeV

preprint2022arXivOpen access
STAR CollaborationM. S. AbdallahB. E. AboonaJ. 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. BunzarovX. 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. 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. KnospeH. S. KoL. KochendaL. K. KosarzewskiL. KramarikP. KravtsovL. KumarS. KumarR. Kunnawalkam ElayavalliJ. H. KwasizurR. LaceyS. LanJ. M. LandgrafJ. LauretA. LebedevR. LednickyJ. H. LeeY. H. LeungC. LiW. LiX. LiY. LiX. LiangY. LiangR. LicenikT. LinY. LinM. A. LisaF. 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. PakJ. PanA. PandavA. K. PandeyY. PanebratsevP. ParfenovB. PawlikD. PawlowskaC. 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. RusnakA. K. SahooN. R. SahooH. SakoS. SalurJ. SandweissS. SatoW. B. SchmidkeN. SchmitzB. R. SchweidF. SeckJ. SegerM. SergeevaR. SetoP. SeybothN. ShahE. ShahalievP. V. ShanmuganathanM. ShaoT. ShaoA. I. SheikhD. Y. 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. 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. 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. XuC. YangQ. YangS. YangY. YangZ. YeL. YiK. YipY. YuH. ZbroszczykW. ZhaC. ZhangD. ZhangJ. ZhangS. ZhangX. P. ZhangY. ZhangZ. J. ZhangZ. ZhangJ. ZhaoC. ZhouX. ZhuM. ZurekM. Zyzak

Abstract

Measurement by the STAR experiment at RHIC of the cold nuclear matter (CNM) effects experienced by inclusive J/ψJ/ψ at mid-rapidity in 0-100\% pp+Au collisions at sNN\sqrt{s_{_{\mathrm{NN}}}} = 200 GeV is presented. Such effects are quantified utilizing the nuclear modification factor, RpAuR_{p\mathrm{Au}}, obtained by taking a ratio of J/ψJ/ψ yield in pp+Au collisions to that in pp+pp collisions scaled by the number of binary nucleon-nucleon collisions. The differential J/ψJ/ψ yield in both pp+pp and pp+Au collisions is measured through the dimuon decay channel, taking advantage of the trigger capability provided by the Muon Telescope Detector in the RHIC 2015 run. Consequently, the J/ψJ/ψ RpAuR_{p\mathrm{Au}} is derived within the transverse momentum (pTp_{\mathrm{T}}) range of 0 to 10 GeV/cc. A suppression of approximately 30% is observed for pT<2p_{\mathrm{T}}<2 GeV/cc, while J/ψJ/ψ RpAuR_{p\mathrm{Au}} becomes compatible with unity for pTp_{\mathrm{T}} greater than 3 GeV/cc, indicating the J/ψJ/ψ yield is minimally affected by the CNM effects at high pTp_{\mathrm{T}}. Comparison to a similar measurement from 0-20% central Au+Au collisions reveals that the observed strong J/ψJ/ψ suppression above 3 Gev/cc is mostly due to the hot medium effects, providing strong evidence for the formation of the quark-gluon plasma in these collisions. Several model calculations show qualitative agreement with the measured J/ψJ/ψ RpAuR_{p\mathrm{Au}}, while their agreement with the J/ψJ/ψ yields in pp+pp and pp+Au collisions is worse.

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