Chiral Magnetic Effect in Hydrodynamic Approximation
Valentin I. Zakharov

TL;DR
This paper reviews the derivation of the chiral magnetic effect within hydrodynamics, emphasizing its non-renormalization and connection to quantum anomalies, and discusses the implications for dissipationless current and potential microscopic mechanisms.
Contribution
It demonstrates that the chiral magnetic effect remains unchanged in hydrodynamics despite strong interactions, using thermodynamics and anomaly theorems, and discusses its quantum and microscopic aspects.
Findings
ChME is not renormalized in hydrodynamics.
The effect is a dissipation-free, ballistic transport phenomenon.
ChME remains unmodified in superfluid conditions.
Abstract
We review derivations of the chiral magnetic effect (ChME) in hydrodynamic approximation. The reader is assumed to be familiar with the basics of the effect. The main challenge now is to account for the strong interactions between the constituents of the fluid. The main result is that the ChME is not renormalized: in the hydrodynamic approximation it remains the same as for non-interacting chiral fermions moving in an external magnetic field. The key ingredients in the proof are general laws of thermodynamics and the Adler-Bardeen theorem for the chiral anomaly in external electromagnetic fields. The chiral magnetic effect in hydrodynamics represents a macroscopic manifestation of a quantum phenomenon (chiral anomaly). Moreover, one can argue that the current induced by the magnetic field is dissipation free and talk about a kind of "chiral superconductivity". More precise description…
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