Identified charged-hadron production in p + Al, 3He +Au, and Cu + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and in U + U collisions at $\sqrt{s_{NN}}$ = 193 GeV

The PHENIX experiment has performed a systematic study of identified charged-hadron ($π^±$, $K^±$, $p$, $\overline{p}$) production at midrapidity in $p$ + Al, 3He +Au, and Cu + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U + U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Identified charged-hadron inv...

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Veröffentlicht in:Physical review. C 2024-05, Vol.109 (5)
Hauptverfasser: Aidala, C., Akiba, Y., Akimoto, R., Alexander, J., Babintsev, V., Bai, M., Bai, X., Bannier, B., Beaumier, M., Campbell, S., Chiu, M., Chi, C. Y., Choi, I. J., Christiansen, P., Connors, M., Corrales Morales, Y., Crossette, N., Dehmelt, K., Denisov, A., Durham, J. M., Fadem, B., Firak, D., Fitzgerald, D., Fleuret, F., Gal, C., Gonin, M., de Cassagnac, R. Granier, Grau, N., Haggerty, J. S., Hayano, R., Hemmick, T. K., Homma, K., Hong, B., Ivanishchev, D., Jacak, B. V., Jezghani, M., Johnson, B. M., Joo, K. S., Kamin, J., Kapustinsky, J., Karthas, S., Kawall, D., Khandai, P. K., Kijima, K. M., Kim, T., Kim, Y. -J., Kitamura, R., Klatsky, J., Kleinjan, D., Koster, J., Larionova, D., Lee, S., Leitch, M. J., Leung, Y. H., Lewis, B., Lökös, S., Lynch, D., Makdisi, Y. I., Mibe, T., Mitsuka, G., Mondal, M. M., Murata, J., Nagae, T., Nakamura, T., Nyanin, A. S., Oh, J., Oide, H., Park, I. H., Park, S. K., Peng, J. -C., Peressounko, D. Yu, Petti, R., Pinson, R., Pisani, R. P., Ravinovich, I., Read, Jr., Kenneth F., Rinn, T., Runchey, J., Shibata, T. -A., Shigaki, K., Shioya, T., Silva, C. L., Skolnik, M., Slunečka, M., Snowball, M., Stepanov, M., Stone, M. R., Sziklai, J., Taketani, A., Tanida, K., Tennant, E., Vazquez-Zambrano, E., Velkovska, J., Watanabe, D., Watanabe, K., White, A. S., Xia, B., Xu, Q., Zajc, W. A., Zhou, S.
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Sprache:eng
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Zusammenfassung:The PHENIX experiment has performed a systematic study of identified charged-hadron ($π^±$, $K^±$, $p$, $\overline{p}$) production at midrapidity in $p$ + Al, 3He +Au, and Cu + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U + U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Identified charged-hadron invariant transverse-momentum ($p_T$) and transverse-mass ($m_T$) spectra are presented and interpreted in terms of radially expanding thermalized systems. The particle ratios of $K/π$ and $p/π$ have been measured in different centrality ranges of large (Cu + Au and U + U) and small ($p$ + Al and 3He +Au) collision systems. The values of $K/π$ ratios measured in all considered collision systems were found to be consistent with those measured in $p + p$ collisions. However, the values of $p/π$ ratios measured in large collision systems reach the values of ≈0.6, which is a factor of ≈2 larger than in $p + p$ collisions. These results can be qualitatively understood in terms of the baryon enhancement expected from hadronization by recombination. Identified charged-hadron nuclear-modification factors ($R_{AB}$) are also presented. Enhancement of proton $R_{AB}$ values over meson $R_{AB}$ values was observed in central 3He +Au, Cu + Au, and U + U collisions. Here, the proton $R_{AB}$ values measured in the $p$ + Al collision system were found to be consistent with $R_{AB}$ values of $Φ$, $π^±$, $K^±$, and $π^0$ mesons, which may indicate that the size of the system produced in $p$ + Al collisions is too small for recombination to cause a noticeable increase in proton production.
ISSN:2469-9985