利用核碰撞追踪重子数

STAR Collaboration
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引用次数: 0

摘要

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。
Tracking the baryon number with nuclear collisions
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.
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