| Institution: | (Fudan University,Shanghai,200433;Lawrence Berkeley National Laboratory,Berkeley,California 94720;Abilene Christian University,Abilene,Texas 79699;Brookhaven National Laboratory,Upton,New York 11973;University of Tsukuba,Tsukuba,Ibaraki 305-8571;Purdue University,West Lafayette,Indiana 47907;Southern Connecticut State University,New Haven,Connecticut 06515;State University of New York,Stony Brook,New York 11794;Rice University,Houston,Texas 77251;Physics Department and Center for Exploration of Energy and Matter,Indiana University,2401 N Milo B.Sampson Lane,Bloomington,IN 47408;College of Physics and Technology,Guangxi Normal University,Guilin,541004;Central China Normal University,Wuhan,Hubei 430079;Ohio State University,Columbus,Ohio 43210;University of Texas,Austin,Texas 78712;University of California,Los Angeles,California 90095;Department of Physics,McGill University,3600 University Street,Montreal,QC,H3A 2T8;Wayne State University,Detroit,Michigan 48201;Huzhou University,Huzhou,Zhejiang 313000) |
| Abstract: | The chiral magnetic effect (CME) is a novel transport phenomenon, arising from the interplay between quantum anomalies and strong magnetic fields in chiral systems. In high-energy nuclear collisions, the CME may survive the expansion of the quark-gluon plasma fireball and be detected in experiments. Over the past two decades, experimental searches for the CME have attracted extensive interest at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC). The main goal of this study is to investigate three pertinent experimental approaches: the \begin{document}$\gamma$\end{document}![]() ![]() correlator, the R correlator, and the signed balance functions. We exploit simple Monte Carlo simulations and a realistic event generator (EBE-AVFD) to verify the equivalence of the core components among these methods and to ascertain their sensitivities to the CME signal and the background contributions for the isobar collisions at the RHIC. |
