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1Yerevan Physics Institute, Yerevan, Armenia.
2Institut für Hochenergiephysik, Wien, Austria.
Eur Phys J C Part Fields. 2018;78(6):509. doi: 10.1140/epjc/s10052-018-5950-6. Epub 2018 Jun 20.
The nuclear modification factors of and mesons are measured in collisions at a centre-of-mass energy per nucleon pair of . The analysis is based on and data samples collected by CMS at the LHC in 2015, corresponding to integrated luminosities of 464 and 28 , respectively. The measurements are performed in the dimuon rapidity range of as a function of centrality, rapidity, and transverse momentum ( ) from in the most forward region and up to 50 . Both prompt and nonprompt (coming from b hadron decays) mesons are observed to be increasingly suppressed with centrality, with a magnitude similar to the one observed at for the two meson components. No dependence on rapidity is observed for either prompt or nonprompt mesons. An indication of a lower prompt meson suppression at is seen with respect to that observed at intermediate . The prompt meson yield is found to be more suppressed than that of the prompt mesons in the entire range.
在每对核子质心能量为 的 碰撞中测量了 和 介子的核修正因子。该分析基于CMS在2015年LHC上收集的 和 数据样本，分别对应于464 和28 的积分亮度。测量在双μ子快度范围 内进行，作为中心度、快度和横向动量（ ）的函数， 从最前沿区域的 到高达50 。观察到即时和非即时（来自b强子衰变） 介子都随着中心度增加而受到越来越大的抑制，其幅度与在 时观察到的两种 介子成分的幅度相似。对于即时或非即时 介子，均未观察到对快度的依赖性。相对于在中间 时观察到的情况，在 时观察到即时 介子抑制较低的迹象。发现在整个 范围内，即时 介子产额比即时 介子产额受到的抑制更大。
