Chiral Magnetic Effect in Heavy Ion Collisions: The Present and Future
arXiv:2405.05427 · doi:10.1142/S0218301324300078
Abstract
The chiral magnetic effect (CME) is a collective quantum phenomenon that arises from the interplay between gauge field topology and fermion chiral anomaly, encompassing a wide range of physical systems from semimetals to quark-gluon plasma. This review, with a focus on CME and related effects in heavy ion collisions, aims to provide an introductory discussion on its conceptual foundation and measurement methodology, a timely update on the present status in terms of experimental findings and theoretical progress, as well as an outlook into the open problems and future developments.
136 pages, 39 figures, book chapter to be included in the Quark-Gluon Plasma 6 edited by Xin-Nian Wang
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Cited by in corpus (11)
- Circularly polarized photon emission from magnetized chiral plasmas
- Search for the chiral magnetic effect through beam energy dependence of charge separation using event shape selection
- Experimental review on the chiral magnetic effect in relativistic heavy ion collisions
- Boundary conditions and electromagnetic effects on the phase transition of a zero spin bosonic system
- Localized Chiral Magnetic Effect in equilibrium QCD
- Berry Curvature and Spin-One Color Superconductivity
- Generalized relativistic second order magnetohydrodynamics: A correlation function approach using Zubarev's nonequilibrium statistical operator
- Chiral vortical conductivities and the moment of inertia of a rigidly rotating Fermi gas
- Photon emission from weakly magnetized neutral pions
- Revisiting the sphaleron and axion production rates in QCD at high temperatures
- Thermal response of the Nieh-Yan term