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$$phi$$ meson production in $$p$$$$+$$Al, $$p$$$$+$$Au, $$d$$$$+$$Au, and $$^3$$He$$+$$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365名*

Acharya, U. A.*; Hasegawa, Shoichi; Imai, Kenichi*; Sako, Hiroyuki; Sato, Susumu; Tanida, Kiyoshi; PHENIX Collaboration*; 365 of others*

Small nuclear collisions are mainly sensitive to cold-nuclear-matter effects; however, the collective behavior observed in these collisions shows a hint of hot-nuclear-matter effects. The identified-particle spectra, especially the $$phi$$ mesons which contain strange and antistrange quarks and have a relatively small hadronic-interaction cross section, are a good tool to study these effects. The PHENIX experiment has measured $$phi$$ mesons in a specific set of small collision systems $$p$$$$+$$Al, $$p$$$$+$$Au, and $$^3$$He$$+$$Au, as well as $$d$$$$+$$Au, at $$sqrt{s_{_{NN}}}=200$$ GeV. The transverse-momentum spectra and nuclear-modification factors are presented and compared to theoretical-model predictions. The comparisons with different calculations suggest that quark-gluon plasma may be formed in these small collision systems at $$sqrt{s_{_{NN}}}=200$$ GeV. However, the volume and the lifetime of the produced medium may be insufficient for observing strangeness-enhancement and jet-quenching effects. Comparison with calculations suggests that the main production mechanisms of $$phi$$ mesons at midrapidity may be different in $$p$$$$+$$Al versus $$p/d/$$$$^3$$He$$+$$Au collisions at $$sqrt{s_{_{NN}}}=200$$ GeV. While thermal quark recombination seems to dominate in $$p/d/$$$$^3$$He$$+$$Au collisions, fragmentation seems to be the main production mechanism in $$p$$$$+$$Al collisions.

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パーセンタイル:69.74

分野:Physics, Nuclear

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