在 $\sqrt{s_\mathrm{NN}}$ = 5.36 TeV 的铅铅对撞中带电强子的伪时态分布

CMS Collaboration
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引用次数: 0

摘要

带电强子的假振幅($\eta$)分布是通过在有史以来最高的核子-核子质心能量$\sqrt{s_\mathrm{NN}}$ = 5.36 TeV下收集的铅-铅离子对撞数据测量的。这些数据由2022年在大型强子对撞机上进行的CMS实验记录,对应于0.30 $\pm$ 0.03 $\mu$b$^{-1}$ 的综合光度。利用CMS硅像素探测器,报告了在$\vert\eta\vert$ $\lt$ 2.6范围内产生的初级带电强子的产率。同时还报告了中速粒子密度的演变与碰撞中心性的函数关系。在5%的最中心碰撞中,发现在$\vert\eta\vert$ $\lt$ 0.5范围内的带电哈德子密度为2032 $\pm$ 91(syst),统计上的不确定性可以忽略不计。这一结果与较低质心能量下的核-核碰撞数据的外推法是一致的。与各种蒙特卡洛事件发生器以及以前在类似碰撞能量下对铅-铅和氙-氙碰撞的测量进行了比较。新数据详细说明了粒子产生与碰撞能量、初始碰撞几何形状和碰撞原子核大小的关系。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Pseudorapidity distributions of charged hadrons in lead-lead collisions at $\sqrt{s_\mathrm{NN}}$ = 5.36 TeV
The pseudorapidity ($\eta$) distributions of charged hadrons are measured using data collected at the highest ever nucleon-nucleon center-of-mass energy of $\sqrt{s_\mathrm{NN}}$ = 5.36 TeV for collisions of lead-lead ions. The data were recorded by the CMS experiment at the LHC in 2022 and correspond to an integrated luminosity of 0.30 $\pm$ 0.03 $\mu$b$^{-1}$. Using the CMS silicon pixel detector, the yields of primary charged hadrons produced in the range $\vert\eta\vert$ $\lt$ 2.6 are reported. The evolution of the midrapidity particle density as a function of collision centrality is also reported. In the 5% most central collisions, the charged-hadron $\eta$ density in the range $\vert\eta\vert$ $\lt$ 0.5 is found to be 2032 $\pm$ 91 (syst), with negligible statistical uncertainty. This result is consistent with an extrapolation from nucleus-nucleus collision data at lower center-of-mass energies. Comparisons are made to various Monte Carlo event generators and to previous measurements of lead-lead and xenon-xenon collisions at similar collision energies. These new data detail the dependence of particle production on the collision energy, initial collision geometry, and the size of the colliding nuclei.
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