Multiplicity Dependent J/ψ and Ψ(2s) Production at Forward and Backward Rapidity in P+p Collisions at √(s)=200 GeV
PHENIX Collaboration,N. J. Abdulameer,U. Acharya,C. Aidala,Y. Akiba,M. Alfred,V. Andrieux,S. Antsupov,N. Apadula,H. Asano,B. Azmoun,V. Babintsev,N. S. Bandara,E. Bannikov,K. N. Barish,S. Bathe,A. Bazilevsky,M. Beaumier,R. Belmont,A. Berdnikov,Y. Berdnikov,L. Bichon,B. Blankenship,D. S. Blau,J. S. Bok,V. Borisov,M. L. Brooks,J. Bryslawskyj,V. Bumazhnov,S. Campbell,R. Cervantes,D. Chen,M. Chiu,C. Y. Chi,I. J. Choi,J. B. Choi,Z. Citron,M. Connors,R. Corliss,N. Cronin,M. Csanád,T. Csörgő,T. W. Danley,M. S. Daugherity,G. David,K. DeBlasio,K. Dehmelt,A. Denisov,A. Deshpande,E. J. Desmond,A. Dion,D. Dixit,V. Doomra,J. H. Do,A. Drees,K. A. Drees,J. M. Durham,A. Durum,H. En'yo,A. Enokizono,R. Esha,B. Fadem,W. Fan,N. Feege,D. E. Fields,M. Jr. Finger,M. Finger,D. Firak,D. Fitzgerald,S. L. Fokin,J. E. Frantz,A. Franz,A. D. Frawley,Y. Fukuda,P. Gallus,C. Gal,P. Garg,H. Ge,F. Giordano,Y. Goto,N. Grau,S. V. Greene,M. Grosse Perdekamp,T. Gunji,T. Guo,H. Guragain,T. Hachiya,J. S. Haggerty,K. I. Hahn,H. Hamagaki,H. F. Hamilton,J. Hanks,S. Y. Han,S. Hasegawa,T. O. S. Haseler,T. K. Hemmick,X. He,J. C. Hill,K. Hill,A. Hodges,R. S. Hollis,K. Homma,B. Hong,T. Hoshino,N. Hotvedt,J. Huang,K. Imai,M. Inaba,A. Iordanova,D. Isenhower,D. Ivanishchev,B. Jacak,M. Jezghani,X. Jiang,Z. Ji,B. M. Johnson,D. Jouan,D. S. Jumper,J. H. Kang,D. Kapukchyan,S. Karthas,D. Kawall,A. V. Kazantsev,V. Khachatryan,A. Khanzadeev,C. Kim,E. -J. Kim,M. Kim,D. Kincses,E. Kistenev,J. Klatsky,P. Kline,T. Koblesky,D. Kotov,L. Kovacs,S. Kudo,K. Kurita,Y. Kwon,J. G. Lajoie,A. Lebedev,S. Lee,M. J. Leitch,Y. H. Leung,S. H. Lim,M. X. Liu,X. Li,V. -R. Loggins,S. Lökös,D. A. Loomis,K. Lovasz,D. Lynch,T. Majoros,Y. I. Makdisi,M. Makek,V. I. Manko,E. Mannel,M. McCumber,P. L. McGaughey,D. McGlinchey,C. McKinney,M. Mendoza,A. C. Mignerey,A. Milov,D. K. Mishra,J. T. Mitchell,M. Mitrankova,Iu. Mitrankov,G. Mitsuka,S. Miyasaka,S. Mizuno,P. Montuenga,T. Moon,D. P. Morrison,B. Mulilo,T. Murakami,J. Murata,K. Nagai,K. Nagashima,T. Nagashima,J. L. Nagle,M. I. Nagy,I. Nakagawa,K. Nakano,C. Nattrass,T. Niida,R. Nouicer,N. Novitzky,T. Novák,G. Nukazuka,A. S. Nyanin,E. O'Brien,C. A. Ogilvie,J. D. Orjuela Koop,M. Orosz,J. D. Osborn,A. Oskarsson,G. J. Ottino,K. Ozawa,V. Pantuev,V. Papavassiliou,J. S. Park,S. Park,M. Patel,S. F. Pate,D. V. Perepelitsa,G. D. N. Perera,D. Yu. Peressounko,C. E. PerezLara,J. Perry,R. Petti,M. Phipps,C. Pinkenburg,R. P. Pisani,M. Potekhin,M. L. Purschke,K. F. Read,D. Reynolds,V. Riabov,Y. Riabov,D. Richford,T. Rinn,S. D. Rolnick,M. Rosati,Z. Rowan,A. S. Safonov,T. Sakaguchi,H. Sako,V. Samsonov,M. Sarsour,S. Sato,B. Schaefer,B. K. Schmoll,K. Sedgwick,R. Seidl,A. Seleznev,A. Sen,R. Seto,A. Sexton,D. Sharma,I. Shein,T. -A. Shibata,K. Shigaki,M. Shimomura,T. Shioya,P. Shukla,A. Sickles,C. L. Silva,D. Silvermyr,B. K. Singh,C. P. Singh,V. Singh,M. Slunečka,K. L. Smith,M. Snowball,R. A. Soltz,W. E. Sondheim,S. P. Sorensen,I. V. Sourikova,P. W. Stankus,S. P. Stoll,T. Sugitate,A. Sukhanov,T. Sumita,J. Sun,Z. Sun,J. Sziklai,K. Tanida,M. J. Tannenbaum,S. Tarafdar,G. Tarnai,R. Tieulent,A. Timilsina,T. Todoroki,M. Tomášek,C. L. Towell,R. S. Towell,I. Tserruya,Y. Ueda,B. Ujvari,H. W. van Hecke,J. Velkovska,M. Virius,V. Vrba,N. Vukman,X. R. Wang,Y. S. Watanabe,C. L. Woody,L. Xue,C. Xu,Q. Xu,S. Yalcin,Y. L. Yamaguchi,H. Yamamoto,A. Yanovich,I. Yoon,J. H. Yoo,I. E. Yushmanov,H. Yu,W. A. Zajc,A. Zelenski,L. Zou
arxiv(2024)
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摘要
The J/ψ and ψ(2S) charmonium states, composed of cc̅ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics in high-energy hadronic interactions. However, there is not yet a complete understanding of the charmonium-production mechanism. Recent measurements of J/ψ production as a function of event charged-particle multiplicity at the collision energies of both the Large Hadron Collider (LHC) and the Relativistic Heavy Ion Collider (RHIC) show enhanced J/ψ production yields with increasing multiplicity. One potential explanation for this type of dependence is multiparton interactions (MPI). We carry out the first measurements of self-normalized J/ψ yields and the ψ(2S) to J/ψ ratio at both forward and backward rapidities as a function of self-normalized charged-particle multiplicity in p+p collisions at √(s)=200 GeV. In addition, detailed pythia studies tuned to RHIC energies were performed to investigate the MPI impacts. We find that the PHENIX data at RHIC are consistent with recent LHC measurements and can only be described by pythia calculations that include MPI effects. The forward and backward ψ(2S) to J/ψ ratio, which serves as a unique and powerful approach to study final-state effects on charmonium production, is found to be less dependent on the charged-particle multiplicity.