Higher-order cumulants and correlation functions of proton multiplicity distributions in sNN=3 GeV Au+Au collisions at the RHIC STAR experiment
Here, we report a measurement of cumulants and correlation functions of event-by-event proton multiplicity distributions from fixed-target Au+Au collisions at $\sqrt{s_\text{NN}}$ = 3 GeV measured by the STAR experiment. Protons are identified within the rapidity (y) and transverse momentum ($p_T$)...
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creator | Adam, J. Adams, J. R. Adkins, J. K. Bellwied, R. Cai, X. Z. Caines, H. Calderón de la Barca Sánchez, M. Chatterjee, A. Chen, Z. Choudhury, S. Chu, X. Crawford, H. J. Csanád, M. Daugherity, M. Dixit, P. Evdokimov, O. Fazio, S. Feng, Y. Geurts, F. Guryn, W. Han, Y. Harrison, H. Herrmann, N. Hu, C. Hu, Y. Huang, T. Huang, Y. Jacobs, W. W. Jia, J. Ju, X. Kabir, M. L. Kang, K. Kauder, K. Keane, D. Kikoła, D. P. Kramarik, L. Kumar, L. Kumar, S. Lan, S. Lauret, J. Li, X. Liu, T. Liu, Y. Ljubicic, T. Llope, W. J. Luo, X. F. Ma, L. Markert, C. Matis, H. S. Mondal, M. M. Nagy, M. I. Nasim, Md Nayak, K. Nelson, J. M. Nishitani, R. Nonaka, T. Odyniec, G. Okubo, K. Pani, T. Pawlik, B. Porter, J. Pruthi, N. K. Quintero, A. Racz, C. Radhakrishnan, S. K. Reed, R. Ruan, L. Schmidke, W. B. Seck, F-J Seger, J. Shah, N. Shen, D. Y. Shen, K. Sichtermann, E. P. Sikora, R. Sinha, P. Stewart, D. J. Sun, C. Sun, X. Tang, A. H. Thomas, J. H. Tribedy, P. Tripathy, S. K. Truhlar, T. Tsang, C. Y. Tu, Z. Upsal, I. Webb, J. C. Westfall, G. D. Wu, X. Xu, Q. H. Yan, Z. Yang, S. Ye, Z. Yip, K. Zha, W. Zhang, J. Zhang, Y. Zhou, J. Zhou, Y. |
description | Here, we report a measurement of cumulants and correlation functions of event-by-event proton multiplicity distributions from fixed-target Au+Au collisions at $\sqrt{s_\text{NN}}$ = 3 GeV measured by the STAR experiment. Protons are identified within the rapidity (y) and transverse momentum ($p_T$) region –0:9 < $\textit{y}$ < 0 and 0:4 < pT < 2:0 GeV/c in the center-of-mass frame. A systematic analysis of the proton cumulants and correlation functions up to sixth-order as well as the corresponding ratios as a function of the collision centrality, $p_T$, and $\textit{y}$ are presented. The effect of pileup and initial volume fluctuations on these observables and the respective corrections are discussed in detail. The results are compared to calculations from the hadronic transport UrQMD model as well as a hydrodynamic model. In the most central 5% collisions, the value of proton cumulant ratio $C_4 = C_2$ is negative, drastically different from the values observed in Au+Au collisions at higher energies. Compared to model calculations including Lattice QCD, a hadronic transport model, and a hydrodynamic model, the strong suppression in the ratio of $C_4/C_2$ at 3 GeV Au+Au collisions indicates an energy regime dominated by hadronic interactions. |
doi_str_mv | 10.1103/PhysRevC.107.024908 |
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R. ; Adkins, J. K. ; Bellwied, R. ; Cai, X. Z. ; Caines, H. ; Calderón de la Barca Sánchez, M. ; Chatterjee, A. ; Chen, Z. ; Choudhury, S. ; Chu, X. ; Crawford, H. J. ; Csanád, M. ; Daugherity, M. ; Dixit, P. ; Evdokimov, O. ; Fazio, S. ; Feng, Y. ; Geurts, F. ; Guryn, W. ; Han, Y. ; Harrison, H. ; Herrmann, N. ; Hu, C. ; Hu, Y. ; Huang, T. ; Huang, Y. ; Jacobs, W. W. ; Jia, J. ; Ju, X. ; Kabir, M. L. ; Kang, K. ; Kauder, K. ; Keane, D. ; Kikoła, D. P. ; Kramarik, L. ; Kumar, L. ; Kumar, S. ; Lan, S. ; Lauret, J. ; Li, X. ; Liu, T. ; Liu, Y. ; Ljubicic, T. ; Llope, W. J. ; Luo, X. F. ; Ma, L. ; Markert, C. ; Matis, H. S. ; Mondal, M. M. ; Nagy, M. I. ; Nasim, Md ; Nayak, K. ; Nelson, J. M. ; Nishitani, R. ; Nonaka, T. ; Odyniec, G. ; Okubo, K. ; Pani, T. ; Pawlik, B. ; Porter, J. ; Pruthi, N. K. ; Quintero, A. ; Racz, C. ; Radhakrishnan, S. K. ; Reed, R. ; Ruan, L. ; Schmidke, W. B. ; Seck, F-J ; Seger, J. ; Shah, N. ; Shen, D. Y. ; Shen, K. ; Sichtermann, E. P. ; Sikora, R. ; Sinha, P. ; Stewart, D. J. ; Sun, C. ; Sun, X. ; Tang, A. H. ; Thomas, J. H. ; Tribedy, P. ; Tripathy, S. K. ; Truhlar, T. ; Tsang, C. Y. ; Tu, Z. ; Upsal, I. ; Webb, J. C. ; Westfall, G. D. ; Wu, X. ; Xu, Q. H. ; Yan, Z. ; Yang, S. ; Ye, Z. ; Yip, K. ; Zha, W. ; Zhang, J. ; Zhang, Y. ; Zhou, J. ; Zhou, Y.</creator><creatorcontrib>Adam, J. ; Adams, J. R. ; Adkins, J. K. ; Bellwied, R. ; Cai, X. Z. ; Caines, H. ; Calderón de la Barca Sánchez, M. ; Chatterjee, A. ; Chen, Z. ; Choudhury, S. ; Chu, X. ; Crawford, H. J. ; Csanád, M. ; Daugherity, M. ; Dixit, P. ; Evdokimov, O. ; Fazio, S. ; Feng, Y. ; Geurts, F. ; Guryn, W. ; Han, Y. ; Harrison, H. ; Herrmann, N. ; Hu, C. ; Hu, Y. ; Huang, T. ; Huang, Y. ; Jacobs, W. W. ; Jia, J. ; Ju, X. ; Kabir, M. L. ; Kang, K. ; Kauder, K. ; Keane, D. ; Kikoła, D. P. ; Kramarik, L. ; Kumar, L. ; Kumar, S. ; Lan, S. ; Lauret, J. ; Li, X. ; Liu, T. ; Liu, Y. ; Ljubicic, T. ; Llope, W. J. ; Luo, X. F. ; Ma, L. ; Markert, C. ; Matis, H. S. ; Mondal, M. M. ; Nagy, M. I. ; Nasim, Md ; Nayak, K. ; Nelson, J. M. ; Nishitani, R. ; Nonaka, T. ; Odyniec, G. ; Okubo, K. ; Pani, T. ; Pawlik, B. ; Porter, J. ; Pruthi, N. K. ; Quintero, A. ; Racz, C. ; Radhakrishnan, S. K. ; Reed, R. ; Ruan, L. ; Schmidke, W. B. ; Seck, F-J ; Seger, J. ; Shah, N. ; Shen, D. Y. ; Shen, K. ; Sichtermann, E. P. ; Sikora, R. ; Sinha, P. ; Stewart, D. J. ; Sun, C. ; Sun, X. ; Tang, A. H. ; Thomas, J. H. ; Tribedy, P. ; Tripathy, S. K. ; Truhlar, T. ; Tsang, C. Y. ; Tu, Z. ; Upsal, I. ; Webb, J. C. ; Westfall, G. D. ; Wu, X. ; Xu, Q. H. ; Yan, Z. ; Yang, S. ; Ye, Z. ; Yip, K. ; Zha, W. ; Zhang, J. ; Zhang, Y. ; Zhou, J. ; Zhou, Y. ; Brookhaven National Laboratory (BNL), Upton, NY (United States)</creatorcontrib><description>Here, we report a measurement of cumulants and correlation functions of event-by-event proton multiplicity distributions from fixed-target Au+Au collisions at $\sqrt{s_\text{NN}}$ = 3 GeV measured by the STAR experiment. Protons are identified within the rapidity (y) and transverse momentum ($p_T$) region –0:9 < $\textit{y}$ < 0 and 0:4 < pT < 2:0 GeV/c in the center-of-mass frame. A systematic analysis of the proton cumulants and correlation functions up to sixth-order as well as the corresponding ratios as a function of the collision centrality, $p_T$, and $\textit{y}$ are presented. The effect of pileup and initial volume fluctuations on these observables and the respective corrections are discussed in detail. The results are compared to calculations from the hadronic transport UrQMD model as well as a hydrodynamic model. In the most central 5% collisions, the value of proton cumulant ratio $C_4 = C_2$ is negative, drastically different from the values observed in Au+Au collisions at higher energies. Compared to model calculations including Lattice QCD, a hadronic transport model, and a hydrodynamic model, the strong suppression in the ratio of $C_4/C_2$ at 3 GeV Au+Au collisions indicates an energy regime dominated by hadronic interactions.</description><identifier>ISSN: 2469-9985</identifier><identifier>EISSN: 2469-9993</identifier><identifier>DOI: 10.1103/PhysRevC.107.024908</identifier><language>eng</language><publisher>United States: American Physical Society (APS)</publisher><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><ispartof>Physical review. 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P.</creatorcontrib><creatorcontrib>Sikora, R.</creatorcontrib><creatorcontrib>Sinha, P.</creatorcontrib><creatorcontrib>Stewart, D. J.</creatorcontrib><creatorcontrib>Sun, C.</creatorcontrib><creatorcontrib>Sun, X.</creatorcontrib><creatorcontrib>Tang, A. H.</creatorcontrib><creatorcontrib>Thomas, J. H.</creatorcontrib><creatorcontrib>Tribedy, P.</creatorcontrib><creatorcontrib>Tripathy, S. K.</creatorcontrib><creatorcontrib>Truhlar, T.</creatorcontrib><creatorcontrib>Tsang, C. Y.</creatorcontrib><creatorcontrib>Tu, Z.</creatorcontrib><creatorcontrib>Upsal, I.</creatorcontrib><creatorcontrib>Webb, J. C.</creatorcontrib><creatorcontrib>Westfall, G. D.</creatorcontrib><creatorcontrib>Wu, X.</creatorcontrib><creatorcontrib>Xu, Q. H.</creatorcontrib><creatorcontrib>Yan, Z.</creatorcontrib><creatorcontrib>Yang, S.</creatorcontrib><creatorcontrib>Ye, Z.</creatorcontrib><creatorcontrib>Yip, K.</creatorcontrib><creatorcontrib>Zha, W.</creatorcontrib><creatorcontrib>Zhang, J.</creatorcontrib><creatorcontrib>Zhang, Y.</creatorcontrib><creatorcontrib>Zhou, J.</creatorcontrib><creatorcontrib>Zhou, Y.</creatorcontrib><creatorcontrib>Brookhaven National Laboratory (BNL), Upton, NY (United States)</creatorcontrib><title>Higher-order cumulants and correlation functions of proton multiplicity distributions in sNN=3 GeV Au+Au collisions at the RHIC STAR experiment</title><title>Physical review. C</title><description>Here, we report a measurement of cumulants and correlation functions of event-by-event proton multiplicity distributions from fixed-target Au+Au collisions at $\sqrt{s_\text{NN}}$ = 3 GeV measured by the STAR experiment. Protons are identified within the rapidity (y) and transverse momentum ($p_T$) region –0:9 < $\textit{y}$ < 0 and 0:4 < pT < 2:0 GeV/c in the center-of-mass frame. A systematic analysis of the proton cumulants and correlation functions up to sixth-order as well as the corresponding ratios as a function of the collision centrality, $p_T$, and $\textit{y}$ are presented. The effect of pileup and initial volume fluctuations on these observables and the respective corrections are discussed in detail. The results are compared to calculations from the hadronic transport UrQMD model as well as a hydrodynamic model. In the most central 5% collisions, the value of proton cumulant ratio $C_4 = C_2$ is negative, drastically different from the values observed in Au+Au collisions at higher energies. Compared to model calculations including Lattice QCD, a hadronic transport model, and a hydrodynamic model, the strong suppression in the ratio of $C_4/C_2$ at 3 GeV Au+Au collisions indicates an energy regime dominated by hadronic interactions.</description><subject>NUCLEAR PHYSICS AND RADIATION PHYSICS</subject><issn>2469-9985</issn><issn>2469-9993</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNo9j81KAzEAhIMoWGqfwEvwKluTTfYnBw9L0bZQqtTitWTz40a2SUmyYh_DN-iz9MlcrXiaj5lhYAC4xmiMMSJ3z80-rNTHZIxRMUYpZag8A4OU5ixhjJHzfy6zSzAK4R0hhHPECowG4Gtm3hrlE-el8lB0267lNgbIrYTCea9aHo2zUHdW_ECATsOdd7H3-m40u9YIE_dQmhC9qbtTyVgYlst7cjxM1evxUHW3Vdfvta0JvzmPMDYKrmbzCXxZVyuoPnfKm62y8QpcaN4GNfrTIVg_Pqwns2TxNJ1PqkXiWBGTFOlCICa0LHXOC06FLKgmJcp4XSMuaJbxQtc4zwhSWmpaUqy1plLWRDKuyRDcnGZdiGYT-g9KNMJZq0Tc4JLRlKXkGzYWbnY</recordid><startdate>20230213</startdate><enddate>20230213</enddate><creator>Adam, J.</creator><creator>Adams, J. 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H. ; Yan, Z. ; Yang, S. ; Ye, Z. ; Yip, K. ; Zha, W. ; Zhang, J. ; Zhang, Y. ; Zhou, J. ; Zhou, Y.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o97t-20f7c09cfd8f6a7a4cd74f3805abb0ac455a7fb16530efdf4841fff4ddb3d9af3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>NUCLEAR PHYSICS AND RADIATION PHYSICS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Adam, J.</creatorcontrib><creatorcontrib>Adams, J. R.</creatorcontrib><creatorcontrib>Adkins, J. K.</creatorcontrib><creatorcontrib>Bellwied, R.</creatorcontrib><creatorcontrib>Cai, X. Z.</creatorcontrib><creatorcontrib>Caines, H.</creatorcontrib><creatorcontrib>Calderón de la Barca Sánchez, M.</creatorcontrib><creatorcontrib>Chatterjee, A.</creatorcontrib><creatorcontrib>Chen, Z.</creatorcontrib><creatorcontrib>Choudhury, S.</creatorcontrib><creatorcontrib>Chu, X.</creatorcontrib><creatorcontrib>Crawford, H. J.</creatorcontrib><creatorcontrib>Csanád, M.</creatorcontrib><creatorcontrib>Daugherity, M.</creatorcontrib><creatorcontrib>Dixit, P.</creatorcontrib><creatorcontrib>Evdokimov, O.</creatorcontrib><creatorcontrib>Fazio, S.</creatorcontrib><creatorcontrib>Feng, Y.</creatorcontrib><creatorcontrib>Geurts, F.</creatorcontrib><creatorcontrib>Guryn, W.</creatorcontrib><creatorcontrib>Han, Y.</creatorcontrib><creatorcontrib>Harrison, H.</creatorcontrib><creatorcontrib>Herrmann, N.</creatorcontrib><creatorcontrib>Hu, C.</creatorcontrib><creatorcontrib>Hu, Y.</creatorcontrib><creatorcontrib>Huang, T.</creatorcontrib><creatorcontrib>Huang, Y.</creatorcontrib><creatorcontrib>Jacobs, W. W.</creatorcontrib><creatorcontrib>Jia, J.</creatorcontrib><creatorcontrib>Ju, X.</creatorcontrib><creatorcontrib>Kabir, M. L.</creatorcontrib><creatorcontrib>Kang, K.</creatorcontrib><creatorcontrib>Kauder, K.</creatorcontrib><creatorcontrib>Keane, D.</creatorcontrib><creatorcontrib>Kikoła, D. P.</creatorcontrib><creatorcontrib>Kramarik, L.</creatorcontrib><creatorcontrib>Kumar, L.</creatorcontrib><creatorcontrib>Kumar, S.</creatorcontrib><creatorcontrib>Lan, S.</creatorcontrib><creatorcontrib>Lauret, J.</creatorcontrib><creatorcontrib>Li, X.</creatorcontrib><creatorcontrib>Liu, T.</creatorcontrib><creatorcontrib>Liu, Y.</creatorcontrib><creatorcontrib>Ljubicic, T.</creatorcontrib><creatorcontrib>Llope, W. J.</creatorcontrib><creatorcontrib>Luo, X. F.</creatorcontrib><creatorcontrib>Ma, L.</creatorcontrib><creatorcontrib>Markert, C.</creatorcontrib><creatorcontrib>Matis, H. S.</creatorcontrib><creatorcontrib>Mondal, M. M.</creatorcontrib><creatorcontrib>Nagy, M. I.</creatorcontrib><creatorcontrib>Nasim, Md</creatorcontrib><creatorcontrib>Nayak, K.</creatorcontrib><creatorcontrib>Nelson, J. M.</creatorcontrib><creatorcontrib>Nishitani, R.</creatorcontrib><creatorcontrib>Nonaka, T.</creatorcontrib><creatorcontrib>Odyniec, G.</creatorcontrib><creatorcontrib>Okubo, K.</creatorcontrib><creatorcontrib>Pani, T.</creatorcontrib><creatorcontrib>Pawlik, B.</creatorcontrib><creatorcontrib>Porter, J.</creatorcontrib><creatorcontrib>Pruthi, N. K.</creatorcontrib><creatorcontrib>Quintero, A.</creatorcontrib><creatorcontrib>Racz, C.</creatorcontrib><creatorcontrib>Radhakrishnan, S. K.</creatorcontrib><creatorcontrib>Reed, R.</creatorcontrib><creatorcontrib>Ruan, L.</creatorcontrib><creatorcontrib>Schmidke, W. B.</creatorcontrib><creatorcontrib>Seck, F-J</creatorcontrib><creatorcontrib>Seger, J.</creatorcontrib><creatorcontrib>Shah, N.</creatorcontrib><creatorcontrib>Shen, D. Y.</creatorcontrib><creatorcontrib>Shen, K.</creatorcontrib><creatorcontrib>Sichtermann, E. P.</creatorcontrib><creatorcontrib>Sikora, R.</creatorcontrib><creatorcontrib>Sinha, P.</creatorcontrib><creatorcontrib>Stewart, D. J.</creatorcontrib><creatorcontrib>Sun, C.</creatorcontrib><creatorcontrib>Sun, X.</creatorcontrib><creatorcontrib>Tang, A. H.</creatorcontrib><creatorcontrib>Thomas, J. H.</creatorcontrib><creatorcontrib>Tribedy, P.</creatorcontrib><creatorcontrib>Tripathy, S. K.</creatorcontrib><creatorcontrib>Truhlar, T.</creatorcontrib><creatorcontrib>Tsang, C. Y.</creatorcontrib><creatorcontrib>Tu, Z.</creatorcontrib><creatorcontrib>Upsal, I.</creatorcontrib><creatorcontrib>Webb, J. C.</creatorcontrib><creatorcontrib>Westfall, G. D.</creatorcontrib><creatorcontrib>Wu, X.</creatorcontrib><creatorcontrib>Xu, Q. H.</creatorcontrib><creatorcontrib>Yan, Z.</creatorcontrib><creatorcontrib>Yang, S.</creatorcontrib><creatorcontrib>Ye, Z.</creatorcontrib><creatorcontrib>Yip, K.</creatorcontrib><creatorcontrib>Zha, W.</creatorcontrib><creatorcontrib>Zhang, J.</creatorcontrib><creatorcontrib>Zhang, Y.</creatorcontrib><creatorcontrib>Zhou, J.</creatorcontrib><creatorcontrib>Zhou, Y.</creatorcontrib><creatorcontrib>Brookhaven National Laboratory (BNL), Upton, NY (United States)</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Physical review. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Adam, J.</au><au>Adams, J. R.</au><au>Adkins, J. K.</au><au>Bellwied, R.</au><au>Cai, X. Z.</au><au>Caines, H.</au><au>Calderón de la Barca Sánchez, M.</au><au>Chatterjee, A.</au><au>Chen, Z.</au><au>Choudhury, S.</au><au>Chu, X.</au><au>Crawford, H. J.</au><au>Csanád, M.</au><au>Daugherity, M.</au><au>Dixit, P.</au><au>Evdokimov, O.</au><au>Fazio, S.</au><au>Feng, Y.</au><au>Geurts, F.</au><au>Guryn, W.</au><au>Han, Y.</au><au>Harrison, H.</au><au>Herrmann, N.</au><au>Hu, C.</au><au>Hu, Y.</au><au>Huang, T.</au><au>Huang, Y.</au><au>Jacobs, W. W.</au><au>Jia, J.</au><au>Ju, X.</au><au>Kabir, M. L.</au><au>Kang, K.</au><au>Kauder, K.</au><au>Keane, D.</au><au>Kikoła, D. P.</au><au>Kramarik, L.</au><au>Kumar, L.</au><au>Kumar, S.</au><au>Lan, S.</au><au>Lauret, J.</au><au>Li, X.</au><au>Liu, T.</au><au>Liu, Y.</au><au>Ljubicic, T.</au><au>Llope, W. J.</au><au>Luo, X. F.</au><au>Ma, L.</au><au>Markert, C.</au><au>Matis, H. S.</au><au>Mondal, M. M.</au><au>Nagy, M. I.</au><au>Nasim, Md</au><au>Nayak, K.</au><au>Nelson, J. M.</au><au>Nishitani, R.</au><au>Nonaka, T.</au><au>Odyniec, G.</au><au>Okubo, K.</au><au>Pani, T.</au><au>Pawlik, B.</au><au>Porter, J.</au><au>Pruthi, N. K.</au><au>Quintero, A.</au><au>Racz, C.</au><au>Radhakrishnan, S. K.</au><au>Reed, R.</au><au>Ruan, L.</au><au>Schmidke, W. B.</au><au>Seck, F-J</au><au>Seger, J.</au><au>Shah, N.</au><au>Shen, D. Y.</au><au>Shen, K.</au><au>Sichtermann, E. P.</au><au>Sikora, R.</au><au>Sinha, P.</au><au>Stewart, D. J.</au><au>Sun, C.</au><au>Sun, X.</au><au>Tang, A. H.</au><au>Thomas, J. H.</au><au>Tribedy, P.</au><au>Tripathy, S. K.</au><au>Truhlar, T.</au><au>Tsang, C. Y.</au><au>Tu, Z.</au><au>Upsal, I.</au><au>Webb, J. C.</au><au>Westfall, G. D.</au><au>Wu, X.</au><au>Xu, Q. H.</au><au>Yan, Z.</au><au>Yang, S.</au><au>Ye, Z.</au><au>Yip, K.</au><au>Zha, W.</au><au>Zhang, J.</au><au>Zhang, Y.</au><au>Zhou, J.</au><au>Zhou, Y.</au><aucorp>Brookhaven National Laboratory (BNL), Upton, NY (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Higher-order cumulants and correlation functions of proton multiplicity distributions in sNN=3 GeV Au+Au collisions at the RHIC STAR experiment</atitle><jtitle>Physical review. C</jtitle><date>2023-02-13</date><risdate>2023</risdate><volume>107</volume><issue>2</issue><issn>2469-9985</issn><eissn>2469-9993</eissn><abstract>Here, we report a measurement of cumulants and correlation functions of event-by-event proton multiplicity distributions from fixed-target Au+Au collisions at $\sqrt{s_\text{NN}}$ = 3 GeV measured by the STAR experiment. Protons are identified within the rapidity (y) and transverse momentum ($p_T$) region –0:9 < $\textit{y}$ < 0 and 0:4 < pT < 2:0 GeV/c in the center-of-mass frame. A systematic analysis of the proton cumulants and correlation functions up to sixth-order as well as the corresponding ratios as a function of the collision centrality, $p_T$, and $\textit{y}$ are presented. The effect of pileup and initial volume fluctuations on these observables and the respective corrections are discussed in detail. The results are compared to calculations from the hadronic transport UrQMD model as well as a hydrodynamic model. In the most central 5% collisions, the value of proton cumulant ratio $C_4 = C_2$ is negative, drastically different from the values observed in Au+Au collisions at higher energies. Compared to model calculations including Lattice QCD, a hadronic transport model, and a hydrodynamic model, the strong suppression in the ratio of $C_4/C_2$ at 3 GeV Au+Au collisions indicates an energy regime dominated by hadronic interactions.</abstract><cop>United States</cop><pub>American Physical Society (APS)</pub><doi>10.1103/PhysRevC.107.024908</doi></addata></record> |
fulltext | fulltext |
identifier | ISSN: 2469-9985 |
ispartof | Physical review. C, 2023-02, Vol.107 (2) |
issn | 2469-9985 2469-9993 |
language | eng |
recordid | cdi_osti_scitechconnect_1894292 |
source | American Physical Society Journals |
subjects | NUCLEAR PHYSICS AND RADIATION PHYSICS |
title | Higher-order cumulants and correlation functions of proton multiplicity distributions in sNN=3 GeV Au+Au collisions at the RHIC STAR experiment |
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