在$\sqrt{s_\mathrm{NN}}$ = 5.02 TeV的pp和\PbPb对撞中利用B$^+$和B$^0_\mathrm{s}$核修正因子计算底夸克能量损失和强子化问题

CMS Collaboration
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The measured\n$p_\\mathrm{T}$-differential cross sections of B$^+$ and B$^0_\\mathrm{s}$ in pp\ncollisions are well described by fixed-order plus next-to-leading logarithm\nperturbative quantum chromodynamics calculations. Using previous PbPb collision\nmeasurements at the same nucleon-nucleon center-of-mass energy, the nuclear\nmodification factors, $R_\\mathrm{AA}$, of the B mesons are determined. For\n$p_\\mathrm{T}$ $\\lt$ 10 GeV/$c$, both mesons are found to be suppressed in PbPb\ncollisions (with $R_\\mathrm{AA}$ values significantly below unity), with less\nsuppression observed for the B$^0_\\mathrm{s}$ mesons. In this $p_\\mathrm{T}$\nrange, the $R_\\mathrm{AA}$ values for the B$^+$ mesons are consistent with\nthose for inclusive charged hadrons and D$^0$ mesons. Below 10 GeV/$c$, both\nB$^+$ and B$^0_\\mathrm{s}$s are found to be less suppressed than either\ninclusive charged hadrons or D$^0$ mesons, with the B$^0_\\mathrm{s}$\n$R_\\mathrm{AA}$ value consistent with unity. 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引用次数: 0

摘要

报告了欧洲核子研究中心大型强子对撞机(CERN LHC)的CMS实验在质心能量为5.02 TeV的质子-质子(pp)对撞中记录的B$^0_\mathrm{s}$和B$^+$介子的产生截面。数据样本对应的综合光度为 302 pb$^{-1}$。截面基于对 B$^0_\mathrm{s}$ $\to$J/$\psi(\mu^+\mu^-)\phi$(1020)(K$^+$K$^-$) 和 B$^+$ $\to$J/\$psi(\mu^+\mu^-)$K$^+$ 衰变通道的测量。结果显示了B介子的横动量($p_\mathrm{T}$)范围为7-50 GeV/$c$,快速性区间为$\lvert y \rvert$ $\lt$ 2.4。在pp对撞中测得的B$^+$和B$^0_\mathrm{s}$的p_\mathrm{T}$-差分截面很好地用固定阶加次对数扰动量子色动力学计算来描述。利用先前在相同核子-核子质心能量下进行的PbPb碰撞测量,确定了B介子的核调制因子$R_\mathrm{AA}$。在p_\mathrm{T}$ $lt$ 10 GeV/$c$的情况下,发现这两种介子在PbPb碰撞中都受到了抑制(R_\mathrm{AA}$的值明显低于统一值),而B$^0_\mathrm{s}$介子受到的抑制较小。在这个$p_\mathrm{T}$范围内,B$^+$介子的$R_\mathrm{AA}$值与包容带电强子和D$^0$介子的值是一致的。在 10 GeV/$c$ 以下,发现 B$^+$ 和 B$^0_\mathrm{s}$ 的抑制程度都低于全包带电强子或 D$^0$ 介子,B$^0_\mathrm{s}$的 $R_\mathrm{AA}$ 值与统一值一致。我们将发现的B$^+$和B$^0_\mathrm{s}$的$R_\mathrm{AA}$值与理论计算结果进行了比较,从而为夸克-胶子等离子体--在超相对论重离子碰撞中产生的高温致密物质--中的底夸克能量损失和加子化机制提供了约束。
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Bottom quark energy loss and hadronization with B$^+$ and B$^0_\mathrm{s}$ nuclear modification factors using pp and \PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV
The production cross sections of B$^0_\mathrm{s}$ and B$^+$ mesons are reported in proton-proton (pp) collisions recorded by the CMS experiment at the CERN LHC with a center-of-mass energy of 5.02 TeV. The data sample corresponds to an integrated luminosity of 302 pb$^{-1}$. The cross sections are based on measurements of the B$^0_\mathrm{s}$ $\to$ J/$\psi(\mu^+\mu^-)\phi$(1020)(K$^+$K$^-$) and B$^+$ $\to$ J/$\psi(\mu^+\mu^-)$K$^+$ decay channels. Results are presented in the transverse momentum ($p_\mathrm{T}$) range 7-50 GeV/$c$ and the rapidity interval $\lvert y \rvert$ $\lt$ 2.4 for the B mesons. The measured $p_\mathrm{T}$-differential cross sections of B$^+$ and B$^0_\mathrm{s}$ in pp collisions are well described by fixed-order plus next-to-leading logarithm perturbative quantum chromodynamics calculations. Using previous PbPb collision measurements at the same nucleon-nucleon center-of-mass energy, the nuclear modification factors, $R_\mathrm{AA}$, of the B mesons are determined. For $p_\mathrm{T}$ $\lt$ 10 GeV/$c$, both mesons are found to be suppressed in PbPb collisions (with $R_\mathrm{AA}$ values significantly below unity), with less suppression observed for the B$^0_\mathrm{s}$ mesons. In this $p_\mathrm{T}$ range, the $R_\mathrm{AA}$ values for the B$^+$ mesons are consistent with those for inclusive charged hadrons and D$^0$ mesons. Below 10 GeV/$c$, both B$^+$ and B$^0_\mathrm{s}$s are found to be less suppressed than either inclusive charged hadrons or D$^0$ mesons, with the B$^0_\mathrm{s}$ $R_\mathrm{AA}$ value consistent with unity. The $R_\mathrm{AA}$ values found for the B$^+$ and B$^0_\mathrm{s}$ are compared to theoretical calculations, providing constraints on the mechanism of bottom quark energy loss and hadronization in the quark-gluon plasma, the hot and dense matter created in ultrarelativistic heavy ion collisions.
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