Nuclear-modification factor of charged hadrons at forward and backward rapidity in pp++Al and pp++Au collisions at sNN=200\sqrt{s_{_{NN}}}=200 GeV

preprint2020arXivOpen access
C. AidalaY. AkibaM. AlfredV. AndrieuxN. ApadulaH. AsanoB. AzmounV. BabintsevN. S. BandaraK. N. BarishS. BatheA. BazilevskyM. BeaumierR. BelmontA. BerdnikovY. BerdnikovD. S. BlauJ. S. BokM. L. BrooksJ. BryslawskyjV. BumazhnovS. CampbellV. Canoa RomanR. CervantesC. Y. ChiM. ChiuI. J. ChoiJ. B. ChoiZ. CitronM. ConnorsN. CroninM. CsanádT. CsörgőT. W. DanleyM. S. DaugherityG. DavidK. DeBlasioK. DehmeltA. DenisovA. DeshpandeE. J. DesmondA. DionD. DixitJ. H. DoA. DreesK. A. DreesJ. M. DurhamA. DurumA. EnokizonoH. En'yoS. EsumiB. FademW. FanN. FeegeD. E. FieldsM. FingerM. Finger, Jr.S. L. FokinJ. E. FrantzA. FranzA. D. FrawleyY. FukudaC. GalP. GallusE. A. GamezP. GargH. GeF. GiordanoY. GotoN. GrauS. V. GreeneM. Grosse PerdekampT. GunjiH. GuragainT. HachiyaJ. S. HaggertyK. I. HahnH. HamagakiH. F. HamiltonS. Y. HanJ. HanksS. HasegawaT. O. S. HaselerX. HeT. K. HemmickJ. C. HillK. HillA. HodgesR. S. HollisK. HommaB. HongT. HoshinoN. HotvedtJ. HuangS. HuangK. ImaiM. InabaA. IordanovaD. IsenhowerS. IshimaruD. IvanishchevB. V. JacakM. JezghaniZ. JiX. JiangB. M. JohnsonD. JouanD. S. JumperJ. H. KangD. KapukchyanS. KarthasD. KawallA. V. KazantsevV. KhachatryanA. KhanzadeevA. KhatiwadaC. KimE. -J. KimM. KimD. KincsesE. KistenevJ. KlatskyP. KlineT. KobleskyD. KotovS. KudoB. KurgyisK. KuritaY. KwonJ. G. LajoieA. LebedevS. LeeS. H. LeeM. J. LeitchY. H. LeungN. A. LewisX. LiS. H. LimM. X. LiuV. -R. LogginsS. LökösK. LovaszD. LynchT. MajorosY. I. MakdisiM. MakekV. I. MankoE. MannelM. McCumberP. L. McGaugheyD. McGlincheyC. McKinneyM. MendozaW. J. MetzgerA. C. MignereyA. MilovD. K. MishraJ. T. MitchellIu. MitrankovG. MitsukaS. MiyasakaS. MizunoP. MontuengaT. MoonD. P. MorrisonS. I. MorrowT. MurakamiJ. MurataK. NagaiK. NagashimaT. NagashimaJ. L. NagleM. I. NagyI. NakagawaK. NakanoC. NattrassS. NelsonT. NiidaR. NishitaniR. NouicerT. NovákN. NovitzkyA. S. NyaninE. O'BrienC. A. OgilvieJ. D. Orjuela KoopJ. D. OsbornA. OskarssonG. J. OttinoK. OzawaV. PantuevV. PapavassiliouJ. S. ParkS. ParkS. F. PateM. PatelW. PengD. V. PerepelitsaG. D. N. PereraD. Yu. PeressounkoC. E. PerezLaraJ. PerryR. PettiM. PhippsC. PinkenburgR. P. PisaniA. PunM. L. PurschkeP. V. RadzevichK. F. ReadD. ReynoldsV. RiabovY. RiabovD. RichfordT. RinnS. D. RolnickM. RosatiZ. RowanJ. RuncheyA. S. SafonovT. SakaguchiH. SakoV. SamsonovM. SarsourS. SatoC. Y. ScarlettB. SchaeferB. K. SchmollK. SedgwickR. SeidlA. SenR. SetoA. SextonD. SharmaI. SheinT. -A. ShibataK. ShigakiM. ShimomuraT. ShioyaP. ShuklaA. SicklesC. L. SilvaD. SilvermyrB. K. SinghC. P. SinghV. SinghM. J. SkobyM. SlunečkaK. L. SmithM. SnowballR. A. SoltzW. E. SondheimS. P. SorensenI. V. SourikovaP. W. StankusS. P. StollT. SugitateA. SukhanovT. SumitaJ. SunZ. SunS. SuzukiJ. SziklaiK. 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. WangZ. WangY. S. WatanabeC. P. WongC. L. WoodyC. XuQ. XuL. XueS. YalcinY. L. YamaguchiH. YamamotoA. YanovichJ. H. YooI. YoonH. YuI. E. YushmanovW. A. ZajcA. ZelenskiY. ZhaiS. ZharkoL. Zou

Abstract

The PHENIX experiment has studied nuclear effects in pp++Al and pp++Au collisions at sNN=200\sqrt{s_{_{NN}}}=200 GeV on charged hadron production at forward rapidity (1.4<η<2.41.4<η<2.4, pp-going direction) and backward rapidity (−2.2<η<−1.2-2.2<η<-1.2, AA-going direction). Such effects are quantified by measuring nuclear modification factors as a function of transverse momentum and pseudorapidity in various collision multiplicity selections. In central pp++Al and pp++Au collisions, a suppression (enhancement) is observed at forward (backward) rapidity compared to the binary scaled yields in pp+pp collisions. The magnitude of enhancement at backward rapidity is larger in pp++Au collisions than in pp++Al collisions, which have a smaller number of participating nucleons. However, the results at forward rapidity show a similar suppression within uncertainties. The results in the integrated centrality are compared with calculations using nuclear parton distribution functions, which show a reasonable agreement at the forward rapidity but fail to describe the backward rapidity enhancement.

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