Measurement of ψ(2S)ψ(2S) nuclear modification at backward and forward rapidity in pp++pp, pp++Al, and pp++Au collisions at sNN=200\sqrt{s_{_{NN}}}=200 GeV

preprint2022arXivOpen access
U. A. AcharyaC. AidalaY. AkibaM. AlfredV. AndrieuxN. ApadulaH. AsanoB. AzmounV. BabintsevN. S. BandaraK. N. BarishS. BatheA. BazilevskyM. BeaumierR. BelmontA. BerdnikovY. BerdnikovL. BichonB. BlankenshipD. S. BlauJ. S. BokV. BorisovM. L. BrooksJ. BryslawskyjV. BumazhnovS. CampbellV. Canoa RomanR. CervantesM. ChiuC. Y. ChiI. J. ChoiJ. B. ChoiZ. CitronM. ConnorsY. Corrales MoralesR. CorlissN. CroninT. CsörgőM. CsanádT. W. DanleyM. S. DaugherityG. DavidC. T. DeanK. DeBlasioK. DehmeltA. DenisovA. DeshpandeE. J. DesmondA. DionD. DixitJ. H. DoV. DoomraA. DreesK. A. DreesJ. M. DurhamA. DurumH. En'yoA. EnokizonoR. EshaS. EsumiB. FademW. FanN. FeegeD. E. FieldsM. Finger, Jr.M. FingerD. FitzgeraldS. L. FokinJ. E. FrantzA. FranzA. D. FrawleyY. FukudaP. GallusC. GalP. GargH. GeM. GilesF. GiordanoY. GotoN. GrauS. V. GreeneM. Grosse PerdekampT. GunjiH. GuragainT. HachiyaJ. S. HaggertyK. I. HahnH. HamagakiH. F. HamiltonJ. HanksS. Y. HanM. HarveyS. HasegawaT. O. S. HaselerT. K. HemmickX. HeJ. C. HillK. HillA. HodgesR. S. HollisK. HommaB. HongT. HoshinoN. HotvedtJ. HuangK. ImaiM. InabaA. IordanovaD. IsenhowerD. IvanishchevB. V. JacakM. JezghaniX. JiangZ. JiB. M. JohnsonD. JouanD. S. JumperJ. H. KangD. KapukchyanS. KarthasD. KawallA. V. KazantsevV. KhachatryanA. KhanzadeevA. KhatiwadaC. KimE. -J. KimM. KimT. KimD. KincsesA. KinganE. KistenevJ. KlatskyP. KlineT. KobleskyD. KotovL. KovacsS. KudoK. KuritaY. KwonJ. G. LajoieD. LarionovaA. LebedevS. LeeS. H. LeeM. J. LeitchY. H. LeungN. A. LewisS. H. LimM. X. LiuX. LiV. -R. LogginsD. A. LoomisK. LovaszD. LynchS. LökösT. MajorosY. I. MakdisiM. MakekV. I. MankoE. MannelM. McCumberP. L. McGaugheyD. McGlincheyC. McKinneyM. MendozaA. C. MignereyA. MilovD. K. MishraJ. T. MitchellM. MitrankovaIu. MitrankovG. MitsukaS. MiyasakaS. MizunoM. M. MondalP. MontuengaT. MoonD. P. MorrisonB. MuliloT. MurakamiJ. MurataK. NagaiK. NagashimaT. NagashimaJ. L. NagleM. I. NagyI. NakagawaK. NakanoC. NattrassS. NelsonT. NiidaR. NouicerT. NovákN. NovitzkyG. NukazukaA. S. NyaninE. O'BrienC. A. OgilvieJ. D. Orjuela KoopJ. D. OsbornA. OskarssonG. J. OttinoK. OzawaV. PantuevV. PapavassiliouJ. S. ParkS. ParkM. PatelS. F. PateW. PengD. V. PerepelitsaG. D. N. PereraD. Yu. PeressounkoC. E. PerezLaraJ. PerryR. PettiM. PhippsC. PinkenburgR. P. PisaniM. PotekhinA. PunM. L. PurschkeP. V. RadzevichN. RamasubramanianK. F. ReadD. ReynoldsV. RiabovY. RiabovD. RichfordT. RinnS. D. RolnickM. RosatiZ. RowanJ. RuncheyA. S. SafonovT. SakaguchiH. SakoV. SamsonovM. SarsourS. SatoB. SchaeferB. K. SchmollK. SedgwickR. SeidlA. SenR. SetoA. SextonD. SharmaI. SheinM. ShibataT. -A. ShibataK. ShigakiM. ShimomuraT. ShioyaP. ShuklaA. SicklesC. L. SilvaD. SilvermyrB. K. SinghC. P. SinghV. SinghM. SlunečkaK. L. SmithM. SnowballR. A. SoltzW. E. SondheimS. P. SorensenI. V. SourikovaP. W. StankusS. P. StollT. SugitateA. SukhanovT. SumitaJ. SunZ. SunJ. SziklaiR. TakahamaK. TanidaM. J. TannenbaumS. TarafdarA. TaranenkoG. TarnaiR. TieulentA. TimilsinaT. TodorokiM. TomášekC. L. TowellR. S. TowellI. TserruyaY. UedaB. UjvariH. W. van HeckeJ. VelkovskaM. ViriusV. VrbaN. VukmanX. R. WangY. S. WatanabeC. P. WongC. L. WoodyL. XueC. XuQ. XuS. YalcinY. L. YamaguchiH. YamamotoA. YanovichI. YoonJ. H. YooI. E. YushmanovH. YuW. A. ZajcA. ZelenskiS. ZharkoL. Zou

Abstract

Suppression of the J/ψJ/ψ nuclear-modification factor has been seen as a trademark signature of final-state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold-nuclear-matter effects until the observation of strong differential suppression of the ψ(2S)ψ(2S) state in p/dp/d++AA collisions suggested the presence of final-state effects. Results of J/ψJ/ψ and ψ(2S)ψ(2S) measurements in the dimuon decay channel are presented here for pp++pp, pp++Al, and pp++Au collision systems at sNN=200\sqrt{s_{_{NN}}}=200 GeV. The results are predominantly shown in the form of the nuclear-modification factor, RpAR_{pA}, the ratio of the ψ(2S)ψ(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in pp++pp collisions. Measurements of the J/ψJ/ψ and ψ(2S)ψ(2S) nuclear-modification factor are compared with shadowing and transport-model predictions, as well as to complementary measurements at Large-Hadron-Collider energies.

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