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The chiral magnetic effect (CME) induces an electric charge separation in a chiral medium along the magnetic field that is mostly produced by spectator protons in heavy-ion collisions. The experimental searches for the CME, based on the charge-dependent angular correlations ($gamma$), however, have remained inconclusive, because the non-CME background contributions are not well understood. Experimentally, the $gamma$ correlators have been measured with respect to the second-order ($Psi_{2}$) and the third-order ($Psi_{3}$) symmetry planes, defined as $gamma_{112}$ and $gamma_{123}$, respectively. The expectation was that with a proper normalization, $gamma_{123}$ would provide a data-driven estimate for the background contributions in $gamma_{112}$. In this work, we calculate different harmonics of the $gamma$ correlators using a charge-conserving version of a multiphase transport (AMPT) model to examine the validity of the said assumption. We find that the pure-background AMPT simulations do not yield an equality in the normalized $gamma_{112}$ and $gamma_{123}$, quantified by $kappa_{112}$ and $kappa_{123}$, respectively. Furthermore, we test another correlator, $gamma_{132}$, within AMPT, and discuss the relation between different $gamma$ correlators.
Because the traditional observable of charge-dependent azimuthal correlator $gamma$ contains both contributions from the chiral magnetic effect (CME) and its background, a new observable of $R_{Psi_{m}}$ has been recently proposed which is expected t
Because the properties of the QCD phase transition and the chiral magnetic effect (CME) depend on the number of quark flavors ($N_{f}$) and quark mass, relativistic heavy-ion collisions provide a natural environment to investigate the flavor features
$alpha$-clustered structures in light nuclei could be studied through snapshots taken by relativistic heavy-ion collisions. A multiphase transport (AMPT) model is employed to simulate the initial structure of collision nuclei and the proceeding colli
Within a multi-phase transport model with string melting scenario, jet transport parameter $hat{q}$ is calculated in Au+Au collisions at $sqrt{s_{NN} } $= 200 GeV and Pb+Pb collisions at $sqrt{s_{NN} } $= 2.76 TeV. The $hat{q}$ increases with the inc
We report the effect of magnetic field on estimation of jet transport coefficient, $hat{q}$ using a simplified quasi-particle model. Our adopted quasi-particle model introduces temperature and magnetic field dependent degeneracy factors of partons, w