\RequirePackage{lineno} %\documentclass[floatfix,twocolumn,showpacs,preprintnumbers,amsmath,amssymb,prl,superscriptaddress]{revtex4} \documentclass[onecolumn,amsmath,amssymb]{revtex4} \usepackage{graphicx}% Include figure files \usepackage{dcolumn}% Align table columns on decimal point \usepackage{bm}% bold math %\usepackage{lineno} \topmargin 1.5 cm \textwidth15cm \textheight 21cm \oddsidemargin0.7cm \columnsep0.2in \pagestyle{empty} \begin{document} %\raggedbottom \title{{\Large Precision measurements of light hypernuclei lifetime and $R_3$ in Au+Au Collisions from STAR experiment}}% Force line breaks with \\ \bigskip \bigskip \author{\large Xiujun Li(USTC), Yuanjing Ji(LBNL) } \affiliation{\normalsize for the STAR Collaboration} \bigskip \bigskip \begin{abstract} \linenumbers %star line number %\begin{linenumbers} \leftskip1.0cm \rightskip1.0cm %\large Hypernuclei are bound nuclear systems of correlated nucleons and hyperons. Therefore, the production of hypernuclei in heavy-ion collisions provides an experimental avenue for studying the hyperon$-$nucleon (Y-N) interaction, which is an important ingredient, not only in the equation-of-state (EoS) of astrophysical objects such as neutron stars but also in the description of the hadronic phase of a heavy-ion collision. The strength of the Y-N interaction can be investigated by measuring the properties of hypernuclei. For example, light $\Lambda$-hypernuclei containing one hyperon are conventionally understood as a weakly bound system of a $\Lambda$ and a nucleus, suggesting their lifetimes are close to the free-$\Lambda$ lifetime. In heavy-ion collisions, light hypernuclei are expected to be abundantly produced at low energies due to the high baryon density. In this poster, we will report precise lifetime measurements of $^3_{\Lambda}H$, $^4_{\Lambda}H$ and $^4_{\Lambda}He$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 3 GeV and 7.2 GeV, recorded by the STAR experiment at RHIC in the fixed-target mode in 2018. We also present the relative branching ratio $R_3$ of $^3_{\Lambda}H$ and $^4_{\Lambda}H$, where $R_3$ is the fraction of the two-body decay rate out of the sum of two-body and three-body decay rates. The results will be compared with model calculations and physics implications will be discussed. \end{abstract} \nolinenumbers % end \maketitle \end{document}