Tracking the baryon number with nuclear collisions

STAR Collaboration
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Abstract

Baryon quantum number is believed to be conserved since baryogenesis in the early Universe. While fractionally charged valence quarks are understood conventionally to each carry a baryon number of 1/3, the baryon junction, a non-perturbative Y-shaped topology of neutral gluons, has also been proposed as an alternative entity tracing the baryon number. Neither scenario has been verified experimentally. The STAR Collaboration reports measurements at mid-rapidity of baryon number ($\boldsymbol{B}$) over the electric charge number difference ($\boldsymbol{\Delta Q}$) in isobar nuclear collisions, and the net-proton yield along rapidity in photonuclear collisions. A larger $\boldsymbol{B/\Delta Q}$ ratio and less asymmetric net-proton yield are observed than predicted from models assigning baryon number to valence quarks. These findings, corroborated by previous measurements in Au+Au collisions, disfavor the valence quark picture.
利用核碰撞追踪重子数
据信,重子量子数自早期宇宙的重子发生以来一直保持不变。虽然人们通常认为带分数电荷的价夸克各自携带的重子数为 1/3,但也有人提出了重子交界处,即中性胶子的非微扰 Y 形拓扑结构,作为追踪重子数的另一种实体。这两种设想都没有得到实验验证。STAR合作组织报告了等边核碰撞中重子数($\boldsymbol{B}$)相对于电荷数差($\boldsymbol{\Delta Q}$)的中速测量结果,以及光子核碰撞中沿快速性的净质子产率。与将重子数赋予价夸克的模型所预测的相比,我们观测到了更大的($\boldsymbol{B/\Delta Q}$)比值和更少的不对称净质子产率。
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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