\documentclass[12pt]{article} \usepackage{geometry} \geometry{a4paper,inner=22mm,outer=22mm,top=26mm,bottom=26mm,} \usepackage{graphicx} \usepackage{authblk} \usepackage{nopageno} \usepackage{lineno} \usepackage[utf8]{inputenc} \usepackage{xcolor} \usepackage{hyperref} \title{(Anti)Hypertriton production and branching ratio measurements in Zr+Zr and Ru+Ru collisions at $\sqrt{s_\mathrm{NN}} = 200\, \mathrm{GeV}$ at STAR} \author{Dongsheng Li (for the STAR Collaboration) \\ University of Science and Technology of China } \begin{document} \maketitle \linenumbers Hypernuclei are bound states of hyperons (Y) and nucleons (N). There have been numerous measurements on hypernuclei yields and intrinsic properties, to investigate their production mechanisms and constrain the Y-N interactions. By contrast, there is significantly less knowledge about antihypernuclei. In 2018, STAR recorded a huge sample of about 4 billion minimum bias events from Zr+Zr and Ru+Ru collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV, enabling precise measurements of the (anti)hypernuclei and tests of the matter-antimatter symmetry. In this contribution, we will present new measurements of (anti)hypertriton yields in Zr+Zr and Ru+Ru collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV, using the two-body and three-body decay channels (${}^{3}_{\Lambda} \mathrm{H} \rightarrow {}^{3}\mathrm{He} + \pi^{-}, {}^{3}_{\Lambda} \mathrm{H} \rightarrow \mathrm{d + p} + \pi^{-}$ and c.c.). The strangeness population factor $\mathrm{S_{3}}$ and $\mathrm{\bar{S}_{3}}$ will be shown as a function of multiplicity, which will help distinguish between different production scenarios. In addition, we will present the ${}^{3}_{\bar{\Lambda}} \mathrm{\bar{H}}/{}^{3}_{\Lambda} \mathrm{H}$ ratio in different collision centralities together with other antiparticle-to-particle ratios, to investigate the matter-antimatter imbalance in Zr+Zr and Ru+Ru collisions. Finally, we will present the first measurement of $\bar{\mathrm{R}}_{3}$, the relative branching ratio of ${}^{3}_{\bar{\Lambda}} \mathrm{\bar{H}}$, which is related to its spin and binding energy. These measurements will provide insight into the internal structure of the (anti)hypertriton. Physics implications on (anti)hypernuclei production mechanism as well as Y-N ($\mathrm{\bar{Y}}$-$\mathrm{\bar{N}}$) interaction will be discussed. \end{document}