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論文

Measurement of the relative yields of $$psi(2S)$$ to $$psi(1S)$$ mesons produced at forward and backward rapidity in $$p+p$$, $$p+$$Al, $$p+$$Au, and $$^3$$He+Au collisions at $$sqrt{s_{NN}}=200$$ GeV

Adare, A.*; 長谷川 勝一; 今井 憲一; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他361名*

Physical Review C, 95(3), p.034904_1 - 034904_10, 2017/03

AA2017-0047.pdf:0.58MB

 被引用回数:15 パーセンタイル:75.53(Physics, Nuclear)

The PHENIX Collaboration has measured the ratio of the yields of $$psi(2S)$$ to $$psi(1S)$$ mesons produced in $$p+p$$, $$p+$$Al, $$p+$$Au, and $$^3$$He+Au collisions at $$sqrt{s_{NN}}=200$$ 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 $$^3$$He-going) direction, the relative yield of $$psi(2S)$$ mesons to $$psi(1S)$$ mesons is consistent with the value measured in $$p+p$$ collisions. However, in the backward (nucleus-going) direction, the $$psi(2S)$$ meson is preferentially suppressed by a factor of $$sim 2$$. This suppression is attributed in some models to the breakup of the weakly bound $$psi(2S)$$ 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.

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