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Baryon-strangeness correlations in Au+Au collisions at s_(NN)~(1/2) = 7.7–200 GeV from the UrQMD model

机译:来自URQMD模型的S_(NN)〜(1/2)〜(1/2)= 7.7-200 GEV的Baryon - 陌生

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摘要

Fluctuations and correlations of conserved charges are sensitive observables for studying the QCD phase transition and critical point in high-energy heavy-ion collisions. We have studied the centrality and energy dependence of mixed cumulants (up to fourth order) between net baryon and net strangeness in Au + Au collisions at s_(NN)~(1/2) = 7.7, 11.5, 19.6, 27, 39, 62.4, and 200 GeV from the ultrarelativistic quantum molecular dynamics (UrQMD) model. To compare with other theoretical calculations, we normalize these mixed cumulants by various order cumulants of net-strangeness distributions. We found that the results obtained from UrQMD calculations are comparable with the results from lattice QCD at low temperature and hadron resonance gas model. The ratios of mixed cumulants (R_(11)~(BS) ,R_(13)~(BS) ,R_(22)~(BS) ,R_(31)~(BS)) from UrQMD calculations show weak centrality dependence. However, themixed-cumulant ratios RBS 11 and R_(31)~(BS) show strong increase at low energy, while the R_(13)~(BS) and R_(22)~(BS) are similar at different energies. Furthermore, we have also studied the correlations between different hadron species and their contributions to the net-baryon and net-strangeness correlations. These model studies can provide baselines for searching for the signals of QCD phase transition and critical point in heavy-ion collisions.
机译:保守电荷的波动和相关性是研究高能量重离子碰撞中的QCD相转变和临界点的敏感观察。我们研究了在S_(nn)〜(1/2)= 7.7,11.5,19.6,27,39,来自Utrarelativistic量子分子动力学(URQMD)模型的62.4和200 GEV。为了与其他理论计算进行比较,我们通过净奇怪分布的各种秩序累积分配来规范这些混合累积剂。我们发现,从URQMD计算获得的结果与低温和HATRON共振气体模型的晶格QCD的结果相当。来自URQMD计算的混合累积剂的比率(R_(11)〜(BS),R_(13)〜(BS),R_(22)〜(BS),R_(31)〜(BS))显示了较弱的中心依赖性。然而,算术累积比RBS 11和R_(31)〜(BS)在低能量下显示出强烈的增加,而R_(13)〜(BS)和R_(22)〜(BS)在不同的能量中类似。此外,我们还研究了不同强子种类之间的相关性及其对Net-Baryon和净陌生的贡献。这些模型研究可以提供用于搜索QCD相变信号和重离子碰撞中的临界点的基线。

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  • 来源
    《Physical Review C》 |2017年第2017期|014914.1-014914.10|共10页
  • 作者单位

    Key Laboratory of Quark and Lepton Physics (MOE) and Institute of Particle Physics Central China Normal University Wuhan 430079 China;

    Key Laboratory of Quark and Lepton Physics (MOE) and Institute of Particle Physics Central China Normal University Wuhan 430079 China;

    School of Physical Sciences National Institute of Science Education and Research HBNI Jatni 752050 India;

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