In the framework of A Multi-Phase Transport (AMPT) model, multi-particle azimuthal cumulant method is used to calculate linear and mode-coupled contributions quadrangular flow harmonic ($v_{4}$), response coefficient as a function centrality in Au+Au collisions at $\sqrt{s_{\mathrm{NN}}}$ = 200, 39, 27 19.6 GeV. This study indicated that $v_{4}$ are sensitive beam energy change. Nevertheless, c...

Energy dependence of specific heat extracted from temperature fluctuation Au + collisions at $\sqrt{{s}_{NN}}$ = 7.7 to 200 GeV was investigated by using a multiphase transport (AMPT) model. The results were compared with those other models and some differences low found. To explain the above describe properties hot dense matter $\sqrt{{s}_{NN}}$, new quantity ${C}_{v}^{*}$ derived for describi...

Transverse spherocity is an event shape observable, which separates the events based on their geometrical shapes. In this work, we use transverse to study identified light flavor production in heavy-ion collisions using A Multi-Phase Transport (AMPT) model. We obtain elliptic flow coefficients for pions, kaons and protons Pb+Pb at $\sqrt{s_{\rm{NN}}} = 5.02$ TeV as a function of collision centr...

A Multi-Phase Transport (AMPT) model is used to investigate the efficacy of several flow observables constrain initial-state deformation Uranium nuclei in U $$+$$ collisions at nucleon–nucleon center-of-mass energy $$\sqrt{\textit{s}_{NN}}$$ = 193 GeV. The multiparticle azimuthal cumulant method sensitivity (I) a set quantities that are sensitive both initial- and final-state effects as well (I...

Although strange quarks are produced in $s\bar{s}$ pairs, the ratio of $\Omega^{-}$ to ${\bar{\Omega}}^{+}$ is greater than one heavy-ion collisions at lower RHIC energies. Thus $\Omega$ hyperons must carry net baryon quantum numbers from colliding nuclei. We present results $K$-$\Omega$ correlations AMPT model simulations Au+Au $\sqrt{s_{NN}}$ = 14.6 GeV, probe dynamics for number transport mi...