用PYTHIA 8.312模拟的p-Pb碰撞中作为 "中心性 "估计的平坦性 Angantyr

Antonio Ortiz, Gyula Bencedi, Feng Fan
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摘要

本文利用PYTHIA 8 Angantyr,研究了在$\sqrt{s_\{rm NN}}=5.02$ TeV的质子引导(p-Pb)碰撞中基于平坦性($\rho$)的 "中心性 "估计。尽管Angantyr仍在发展之中,但现有的实施方案足以研究不存在中等效应的系统中的粒子产生。首先,将ALICE数据中的伪振型分布作为前向倍率(V0M)的函数,以及非单衍射p-Pbcollisions中已识别粒子的横动量分布与Angantyr进行了比较。其次,比较了不同 "中心性 "估计器的双核子-核子($N_{\rm coll}$)碰撞的平均次数。研究包括以下 "中心性 "估计器:V0M、$\rho$和中速多重性(CL1)。一方面,$\langle N_{\rm coll} 的 "中心性 "依赖于$\rangle$。一方面,$\rho$选择的 "中心性 "依赖于$\langle N_{\rm coll},与使用影响参数$b$得到的结果相比,显示出最小的偏差(<8%);另一方面,V0M和CL1与使用$b$得到的结果相比,产生了巨大的偏差(最多为2倍)。我们还研究了粒子比和核修正因子($Q_{\rm pPb}$)与$p_{\rm T}$的函数关系。质子与负离子的比值在中间的$p_{\rm T}$(2-8 GeV/$c$)处表现出一个类似流动的峰值,对于V0M、$\rho$和$b$的选择来说,几乎不存在 "中心性 "依赖。对于同样的选择,高子与负离子的比值与$p_{\rm T}$的函数 "中心性 "无关。相反,对于 CL1 类,其比率表现出与硬物理学相关的典型行为。关于$Q_{\rm pPb}$,当用$b$或$\rho$获得 "中心性 "时,在不同粒子种类的中间$p_{\rm T}$(2-8$ GeV/$c$)处观察到一个峰值。在基于 V0M 和 CL1 的选择中,观察到的特征有所减弱。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flattenicity as "centrality" estimator in p-Pb collisions simulated with PYTHIA 8.312 Angantyr
In this paper, a "centrality" estimator based on flattenicity ($\rho$) is studied in proton-led (p-Pb) collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV using PYTHIA 8 Angantyr. Although Angantyr is still under development, the existing implementation is enough to study the particle production in systems where medium effects are absent. Firstly, ALICE data on pseudorapidity distributions as a function of the forward multiplicity (V0M), as well as transverse momentum distributions of identified particles in non-single diffractive p-Pb collisions, are compared with Angantyr. Secondly, the average number of binary nucleon-nucleon ($N_{\rm coll}$) collisions for different "centrality" estimators are compared. The studies include the following "centrality" estimators: V0M, $\rho$ and midrapidity multiplicity (CL1). On one hand, the "centrality" dependence of $\langle N_{\rm coll} \rangle$ for the $\rho$ selection shows the smallest deviations ($<8$ %) with respect to that obtained using impact parameter $b$; on the other hand, the V0M and CL1 yield huge deviations (up to a factor 2) with respect to the results using $b$. The particle ratios and nuclear modification factors ($Q_{\rm pPb}$) as a function of $p_{\rm T}$ are also studied. The proton-to-pion ratio exhibits a flow-like peak at intermediate $p_{\rm T}$ (2-8 GeV/$c$) with little or no "centrality" dependence for V0M, $\rho$ and $b$ selections. The kaon-to-pion ratio as a function of $p_{\rm T}$ is "centrality" independent for the same selections. On the contrary, for the CL1 class the ratios exhibit the typical behaviour associated with hard physics. Regarding $Q_{\rm pPb}$, a peak at intermediate $p_{\rm T}$ ($2-8$ GeV/$c$) for different particle species is observed when the "centrality" is obtained with $b$ or $\rho$. The observed features diminish for the selections based on V0M and CL1.
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