6533b7dbfe1ef96bd1270889
RESEARCH PRODUCT
Measurement of the relative yields of ψ(2S) to ψ(1S) mesons produced at forward and backward rapidity in p+p , p+Al , p+Au , and He3+Au collisions at sNN=200 GeV
P. L. McgaugheyT. MurakamiS. BeckmanS. HasegawaS. I. MorrowY. J. KwonX. HeA. FranzJ. RuncheyV. BumazhnovN. FeegeB. KomkovM. RosatiA. V. KazantsevM. L. KimballY. FukudaMin Soo KimMin Soo KimL. ZouG. TarnaiAlexander MilovB. M. JohnsonB. M. JohnsonP. SettTamás CsörgőNorio SaitoMaya Hachiya ShimomuraMaya Hachiya ShimomuraR. S. HollisMinghui LiuM. ViriusD. DixitY. UedaB. AzmounKenneth Francis ReadKenneth Francis ReadI. NakagawaS. KudoSerpil YalcinJ. D. Orjuela KoopC. H. ChenY. I. MakdisiN. N. AjitanandH. MasudaKensuke HommaS. TarafdarS. TarafdarC. ButlerTaku GunjiTakafumi NiidaJ. HuangM. ChiuAgneta OskarssonM. PatelJohn Matthew DurhamA. ManionG. D. N. PereraKenichi ImaiC. L. SilvaY. BerdnikovS. H. LeeY. AkibaT. O. S. HaselerP. KlineP. B. DissC. MckinneyC. A. OgilvieC. P. WongD. P. MorrisonJohn HillT. K. HemmickJiangyong JiaJiangyong JiaY. GotoVaclav VrbaVaclav VrbaK. HillR. S. TowellA. DionT. ShioyaV. BabintsevTatsuya ChujoT. Sugitate45G. MitsukaX. JiangShunji NishimuraK. A. DreesHideki HamagakiW. FanK. AokiG. DavidK. I. HahnM. ConnorsW. A. ZajcPrakhar GargPrakhar GargB. BannierT. NovákM. J. TannenbaumD. KincsesBrajesh K. SinghG. J. OttinoJen-chieh PengJ. G. RubinB. J. RamsonH. NakagomiT. HoshinoJ. E. FrantzD. KleinjanD. LynchV. R. LogginsL. XueA. DenisovYuki WatanabeA. DurumS. CampbellS. CampbellB. K. SchmollA. MwaiM. I. NagySergey FokinR. S. TowellA. SenA. SenM. MalaevA. TaketaniPrashant ShuklaMartin PurschkeK. DeblasioD. ReynoldsC. A. AidalaA. S. SafonovXiong WangSenta GreeneC. AyusoJaehyeok YooM. StepanovHari GuragainA. MelesS. F. PateK. NagaiY. RiabovY. RiabovN. CroninN. CroninKenta ShigakiR. CervantesK. LovaszJ. KlatskyA. SukhanovK. KuritaDong Jo KimJ. H. DoC. KimC. KimC. L. TowellY. L. YamaguchiY. L. YamaguchiB. SahlmuellerE. J. MannelT. RinnM. TomášekA. EnokizonoY. ItoPawan Kumar NetrakantiR. PinsonM. MendozaA. S. NyaninI. RavinovichJ. A. KeyJ. HanksHiroyuki SakoS. Vazquez-carsonRachid NouicerA. N. ZelenskiKiyoshi TanidaKiyoshi TanidaE. K. BownesK. L. SmithJ. BryslawskyjJ. BryslawskyjZ. RowanV. R. LogginsJ. T. MitchellB. FademE. O'brienS. KandaD. E. FieldsB. V. JacakRadek NovotnyN. HotvedtW. PengP. W. StankusR. SeidlA. TaranenkoVladislav MankoV. AndrieuxM. BaiAlice MignereyN. VukmanH. YuH. YuV. KhachatryanE. KistenevC. XuH. GeJ. A. SilvaS. MizunoM. WysockiR. A. SoltzK. NakanoY. H. LeungM. SlunečkaC. L. WoodyA. BerdnikovMotoi InabaW. E. SondheimM. BeaumierS. MiyasakaM. SarsourP. YinC. PinkenburgAnimesh DattaT. SumitaC. Y. ChiMate CsanadA. IordanovaJ. R. KotlerD. IvanishchevI. TserruyaM. Grosse PerdekampE. O. LallowM. JezghaniK. BoyleByung-sik HongA. DeshpandeH. YamamotoK. DehmeltS. D. RolnickA. R. MendezH. W. Van HeckeV. SinghR. PakZ. WangA. SextonA. BazilevskyJ. SunTakao SakaguchiS. Y. HanV. PapavassiliouPetr GallusF. GiordanoS. ZhouP. MontuengaT. KobleskyT. NagashimaD. McglincheyF. WeiT. ElderQiao XuJ. D. OsbornM. KurosawaInseok YoonC. E. PerezlaraD. SilvermyrR. SetoT. W. DanleyA. D. FrawleyAlexandre LebedevK. OzawaN. GrauI. V. SourikovaS. EsumiM. FingerA. TimilsinaH. En'yoM. J. LeitchS. H. LimS. H. LimA. YanovichA. TakedaA. S. WhiteKoji SatoA. GlennEunja KimS. HuangJ. S. ParkJ. S. ParkM. BoerN. ApadulaN. ApadulaA. DreesN. NovitzkyN. NovitzkyR. P. PisaniK. N. BarishH. StienJ. H. KangJ. S. HaggertyR. BelmontR. BelmontS. ZharkoS. SyedS. KarthasH. F. HamiltonD. KotovD. KotovY. WatanabeKei NagashimaZ. JiD. Yu PeressounkoM. MccumberV. PantuevA. PunB. KimelmanD. S. JumperS. P. StollK. HashimotoD. V. PerepelitsaD. V. PerepelitsaV. Canoa RomanG. W. KimJ. P. DusingC. GalXingguo LiM. L. BrooksJ. ImrekRaphael Noel TieulentD. KapukchyanC. J. PressSusumu SatoR. KitamuraH. AsanoS. P. SorensenAjit Kumar MohantyT. A. ShibataD. JouanJulia VelkovskaD. IsenhowerT. MoonD. KawallJ. G. LajoieM. AlfredT. HachiyaMichael William PhippsMichael William PhippsL. D. LiuViktor RiabovViktor RiabovS. LeeJennifer E. PerryM. S. DaugherityC. P. SinghN. A. LewisR. J. PettiR. J. PettiV. JorjadzeJ. SziklaiS. ParkS. ParkJ. MurataZvi Hirsh CitronI. SheinM. SnowballI. J. ChoiS. BatheB. XiaK. SedgwickMihael MakekN. S. BandaraVladimir SamsonovVladimir SamsonovChristine NattrassT. TodorokiJ. L. NagleD. SharmaD. RichfordAnne Marie SicklesAnne Marie SicklesB. SchaeferJ. S. BokT. MajorosJan RakR. LaceyA. AdareD. E. MihalikAlexei KhanzadeevJ. B. ChoiDipak Kumar MishraT. V. MoukhanovaMirta DumancicDmitry BlauE. J. DesmondBalazs UjvariI. E. Yushmanovsubject
PhysicsParticle physicsMeson010308 nuclear & particles physicsBranching fractionHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQuarkonium01 natural sciencesDeconfinementNuclear physicsExcited state0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsGlauberdescription
The PHENIX Collaboration has measured the ratio of the yields of ψ(2S) to ψ(1S) mesons produced in p+p, p+Al, p+Au, and He3+Au collisions at sNN=200 GeV over the forward and backward rapidity intervals 1.2<|y|<2.2. We find that the ratio in p+p collisions is consistent with measurements at other collision energies. In collisions with nuclei, we find that in the forward (p-going or He3-going) direction, the relative yield of ψ(2S) mesons to ψ(1S) mesons is consistent with the value measured in p+p collisions. However, in the backward (nucleus-going) direction, the ψ(2S) meson is preferentially suppressed by a factor of ∼2. This suppression is attributed in some models to the breakup of the weakly bound ψ(2S) meson through final-state interactions with comoving particles, which have a higher density in the nucleus-going direction. These breakup effects may compete with color screening in a deconfined quark-gluon plasma to produce sequential suppression of excited quarkonia states.
year | journal | country | edition | language |
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2017-03-09 | Physical Review C |