Baryon and electric charge stoppings in nuclear collisions and the role of strangeness

TL;DR

This paper investigates baryon and electric charge stopping in nuclear collisions, emphasizing the role of strangeness asymmetry and comparing model predictions with experimental data to understand particle distributions.

Contribution

It highlights the sensitivity of the $B/Q\times Z/A$ ratio to strange-antistrange asymmetry and challenges existing models with recent STAR data.

Findings

The $B/Q\times Z/A$ ratio depends strongly on $s-\bar s$ asymmetry.

AMPT model predicts ratios inconsistent with STAR data without considering asymmetry.

The $B/\Delta Q\times \Delta Z/A$ ratio is sensitive to light quark stopping.

Abstract

It has been challenging to quantitatively understand the stopping of incoming nucleons in nuclear collisions, and recently it has been proposed that comparing the baryon stopping with electric charge stopping can help address the question. Here we focus on the $B/Q\times Z/A$ ratio, which can strongly depend on rapidity although its value is one for the full phase space. We find that this ratio is very sensitive to the difference between strange and anti-strange rapidity distributions (the $s-\bar s$ asymmetry), and slightly more anti-strange quarks at mid-rapidity would lead to a ratio well below one. This is the case for Zr+Zr and Ru+Ru isobar collisions at $200A$ GeV from a multi-phase transport (AMPT) model. Without the $s-\bar s$ asymmetry, the AMPT model would give a mid-rapidity $B/Q\times Z/A$ ratio at or above one. In addition, the AMPT model gives $B/\Delta Q\times \Delta Z/A<1$ at mid-rapidity for isobar collisions at all centralities, which strongly contradicts the recent data from the STAR Collaboration. We further find that the $B/\Delta Q\times \Delta Z/A$ ratio is very sensitive to the net-light quark ($u,d$) stoppings, but it is less sensitive to the $s-\bar s$ asymmetry than the $B/Q\times Z/A$ ratio by a factor of 3.