Measurement of psi(2S) nuclear modification at backward and forward rapidity in p plus p, p plus Al, and p plus Au collisions at root sNN=200 GeV

U. A. Acharya, C. Aidala,Y. Akiba,M. Alfred,V. Andrieux,N. Apadula,H. Asano,B. Azmoun, V. Babintsev,N. S. Bandara,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,V. Canoa Roman,R. Cervantes,M. Chiu,C. Y. Chi,I. J. Choi,J. B. Choi,Z. Citron,M. Connors,Y. Corrales Morales,R. Corliss, N. Cronin,T. Csörgő,M. Csanád,T. W. Danley,M. S. Daugherity, G. David, C. T. Dean,K. DeBlasio,K. Dehmelt,A. Denisov,A. Deshpande,E. J. Desmond,A. Dion,D. Dixit,J. H. Do,V. Doomra,A. Drees,K. A. Drees,J. M. Durham,A. Durum,H. En'yo,A. Enokizono,R. Esha,S. Esumi,B. Fadem,W. Fan,N. Feege,D. E. Fields,M. Finger Jr.,M. Finger,D. Fitzgerald,S. L. Fokin,J. E. Frantz,A. Franz,A. D. Frawley,Y. Fukuda, P. Gallus,C. Gal,P. Garg,H. Ge,M. Giles,F. Giordano,Y. Goto, N. Grau, S. V. Greene,M. Grosse Perdekamp,T. Gunji,H. Guragain,T. Hachiya,J. S. Haggerty,K. I. Hahn, H. Hamagaki,H. F. Hamilton,J. Hanks,S. Y. Han,M. Harvey,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. V. 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,A. Khatiwada,C. Kim, E. -J. Kim,M. Kim, T. Kim,D. Kincses,A. Kingan,E. Kistenev,J. Klatsky,P. Kline,T. Koblesky,D. Kotov,L. Kovacs, S. Kudo,K. Kurita, Y. Kwon,J. G. Lajoie,D. Larionova,A. Lebedev,S. Lee,S. H. Lee,M. J. Leitch,Y. H. Leung,N. A. Lewis,S. H. Lim,M. X. Liu,X. Li,V. -R. Loggins,D. A. Loomis,K. Lovasz,D. Lynch,S. Lökös,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,M. M. Mondal,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,S. Nelson,T. Niida,R. Nouicer,T. Novák,N. Novitzky,G. Nukazuka,A. S. Nyanin,E. O'Brien,C. A. Ogilvie,J. D. Orjuela Koop,J. D. Osborn,A. Oskarsson,G. J. Ottino,K. Ozawa,V. Pantuev, V. Papavassiliou,J. S. Park,S. Park,M. Patel,S. F. Pate,W. Peng,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,A. Pun,M. L. Purschke,P. V. Radzevich,N. Ramasubramanian,K. F. Read,D. Reynolds, V. Riabov,Y. Riabov,D. Richford,T. Rinn,S. D. Rolnick,M. Rosati,Z. Rowan,J. Runchey,A. S. Safonov, T. Sakaguchi,H. Sako,V. Samsonov,M. Sarsour,S. Sato,B. Schaefer,B. K. Schmoll,K. Sedgwick,R. Seidl,A. Sen, R. Seto,A. Sexton,D. Sharma,I. Shein, M. Shibata, 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,R. Takahama, K. Tanida,M. J. Tannenbaum,S. Tarafdar,A. Taranenko,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. P. Wong,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, S. Zharko,L. Zou

PHYSICAL REVIEW C(2022)

引用 2|浏览41
暂无评分
摘要
Suppression of the J/psi 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 psi(2S) state in p + A and d + A collisions suggested the presence of final-state effects. Results of J/psi and psi(2S) measurements in the dimuon decay channel are presented here for p + p, p + Al, and p + Au collision systems at root sNN = 200 GeV. The results are predominantly shown in the form of the nuclear-modification factor, R-pA, the ratio of the psi(2S) invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in p + p collisions. Measurements of the J/psi and psi(2S) nuclear-modification factor are compared with shadowing and transport-model predictions, as well as to complementary measurements at Large Hadron Collider energies.
更多
查看译文
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要