ﻻ يوجد ملخص باللغة العربية
A precise measurement of the hypertriton lifetime is presented. In this letter, the mesonic decay modes $mathrm{{^3_Lambda}H rightarrow ^3He + pi^-}$ and $mathrm{{^3_Lambda}H rightarrow d + p + pi^-}$ are used to reconstruct the hypertriton from Au+Au collision data collected by the STAR collaboration at RHIC. A minimum $chi^2$ estimation is used to determine the lifetime of $tau = 142^{+24}_{-21},{rm (stat.)} {pm} 31,{rm (syst.)}$ ps. This lifetime is about 50% shorter than the lifetime $tau = 263pm2$ ps of a free $Lambda$, indicating strong hyperon-nucleon interaction in the hypernucleus system. The branching ratios of the mesonic decay channels are also determined to satisfy B.R.$_{(^3{rm He}+pi^-)}/$(B.R.$_{(^3{rm He}+pi^-)}+$B.R.$_{(d+p+pi^-)})$ = $0.32rm{pm}0.05,{rm (stat.)}pm 0.08,{rm (syst.)}$. Our ratio result favors the assignment $J(mathrm{^{3}_{Lambda}H})$ = $frac{1}{2}$ over $J(mathrm{^{3}_{Lambda}H})$ = $frac{3}{2}$. These measurements will help to constrain models of hyperon-baryon interactions.
We report a systematic measurement of cumulants, $C_{n}$, for net-proton, proton and antiproton multiplicity distributions, and correlation functions, $kappa_n$, for proton and antiproton multiplicity distributions up to the fourth order in Au+Au col
We analyze the transverse momentum distribution of $J/psi$ mesons produced in Au + Au collisions at the top RHIC energy within a blast-wave model that accounts for a possible inhomogeneity of the charmonium distribution and/or flow fluctuations. The
An excitation function of proton rapidity distributions for different centralities is reported from AGS Experiment E917 for Au+Au collisions at 6, 8, and 10.8 GeV/nucleon. The rapidity distributions from peripheral collisions have a valley at midrapi
Reconstructed jets in heavy ion collisions are a crucial tool for understanding the quark-gluon plasma. The separation of jets from the underlying event is necessary particularly in central heavy ion reactions in order to quantify medium modification
Different orientations of $alpha$-clustered carbon nuclei colliding with heavy ions can result in a large variation in the value of anisotropic flow. Thus, photon flow observables from clustered ${rm^{12}C}$ and ${rm^{197}Au}$ collisions could be a p