Measurement of beauty production via non-prompt charm hadrons in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV

ALICE Collaboration
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Abstract

The production cross sections of $\mathrm {D^0}$, $\mathrm {D^+}$, and $\mathrm {\Lambda_{c}^{+}}$ hadrons originating from beauty-hadron decays (i.e. non-prompt) were measured for the first time at midrapidity in proton$-$lead (p$-$Pb) collisions at the center-of-mass energy per nucleon pair of $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV. Nuclear modification factors ($R_{\mathrm {pPb}}$) of non-prompt $\mathrm {D^0}$, $\mathrm {D^+}$, and $\mathrm {\Lambda_{c}^{+}}$ are calculated as a function of the transverse momentum ($p_{\mathrm T}$) to investigate the modification of the momentum spectra measured in p$-$Pb collisions with respect to those measured in proton$-$proton (pp) collisions at the same energy. The $R_{\mathrm {pPb}}$ measurements are compatible with unity and with the measurements in the prompt charm sector, and do not show a significant $p_{\mathrm T}$ dependence. The $p_{\mathrm T}$-integrated cross sections and $p_{\mathrm T}$-integrated $R_{\mathrm {pPb}}$ of non-prompt $\mathrm {D^0}$ and $\mathrm {D^+}$ mesons are also computed by extrapolating the visible cross sections down to $p_{\mathrm T}$ = 0. The non-prompt D-meson $R_{\mathrm {pPb}}$ integrated over $p_{\mathrm T}$ is compatible with unity and with model calculations implementing modification of the parton distribution functions of nucleons bound in nuclei with respect to free nucleons. The non-prompt $\mathrm {\Lambda_{c}^{+}/D^{0}}$ and $\mathrm{D^+/D^0}$ production ratios are computed to investigate hadronisation mechanisms of beauty quarks into mesons and baryons. The measured ratios as a function of $p_{\mathrm T}$ display a similar trend to that measured for charm hadrons in the same collision system.
在$\sqrt{s_{mathrm{NN}}} = 5.02$ TeV的p-Pb对撞中通过非突变粲强子测量美的产生
在质子$-$lead(p$-$Pb)对撞中,在每个核子对的质量中心能量为$\sqrt{p$-$Pb的条件下,首次测量了$\mathrm {D^0}$, $\mathrm {D^+}$, 和$\mathrm {Lambda_{c}^{+}$ 中子的产生截面。首次在质子$-铅(p$-Pb)对撞中,在每个核子对的质量中心能量$\sqrt{s_\{mathrm{NN}} = 5.02$ TeV下测量了非突变的强子。非突变$\mathrm {D^0}$, $\mathrm {D^+}$ 的核修正因子($R_{mathrm{pPb}}$)、和 $\mathrm {Lambda_{c}^{+}$ 是作为横动量($p_{\mathrm T}$)的函数来计算的,以研究在相同能量下,p$-$Pb 对撞中测得的动量谱与质子$-$质子(pp)对撞中测得的动量谱之间的变化。$R_{\mathrm {pPb}}$ 测量值与统一值以及瞬时粲部门的测量值一致,并且没有显示出显著的$p_{mathrm T}$ 依赖性。通过将可见截面外推到$p_{/\mathrm T}$ =0,我们还计算了非瞬发$\mathrm {D^0}$ 和$\mathrm {D^+}$ 介子的$p_{/\mathrm T}$ 积分截面和$p_{/\mathrm T}$ 积分$R_{/\mathrm{pPb}}$。在 $p_{{m\mathrm T}$ 上积分的非即期 D 介子 $R_{{m\mathrm {pPb}}$ 与统一性相一致,也与模型计算中对束缚在核子中的核子相对于自由核子的部分子分布函数的修改相一致。计算了非突变$\mathrm {\Lambda_{c}^{+}/D^{0}$ 和$\mathrm{D^+/D^0}$ 产生比,以研究美夸克变成介子和重子的强子化机制。作为$p_{\mathrm T}$函数的测量比率显示出与同一碰撞系统中粲中子的测量结果相似的趋势。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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