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論文

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

Acharya, U. A.*; 長谷川 勝一; 今井 憲一*; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他310名*

Physical Review C, 105(6), p.064912_1 - 064912_15, 2022/06

 被引用回数:19 パーセンタイル:89.94(Physics, Nuclear)

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 $$p/d$$$$+$$$$A$$ 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 $$sqrt{s_{_{NN}}}=200$$ 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.

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