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Chiral Magnetic Wave

Dmitri E. Kharzeev, Ho-Ung Yee

TL;DR

This work demonstrates that triangle anomalies in magnetized relativistic plasmas generate a new gapless collective mode, the Chiral Magnetic Wave (CMW), coupling electric and chiral charge density waves and propagating along the magnetic field. It derives and cross-validates the CMW across three frameworks: relativistic magnetohydrodynamics, strong-field dimensional reduction to a 1+1D Sine-Gordon description, and holographic QCD via the Sakai–Sugimoto model, revealing a nonperturbative, field-dependent wave velocity that approaches the speed of light at large $eB$. By incorporating dynamical electromagnetism, the study shows how CMW mixes with plasmons, altering plasmon dispersions and yielding Schwinger-type photon masses in strong fields. The results have potential implications for heavy-ion collision phenomenology, including reaction-plane dependent charge fluctuations, and establish a robust, multi-method confirmation of the CMW across weak and strong coupling regimes.

Abstract

We consider a relativistic plasma containing charged chiral fermions in an external magnetic field, e.g a chirally symmetric quark-gluon plasma created in relativistic heavy ion collisions. We show that triangle anomalies imply the existence of a new type of collective gapless excitation in this system that stems from the coupling between the density waves of the electric and chiral charges; we call it "the Chiral Magnetic Wave" (CMW). The CMW exists even in a neutral plasma, i.e. in the absence of the axial and vector chemical potentials. We demonstrate the existence of CMW and study its properties using three different approaches: i) relativistic magnetohydrodynamics; ii) dimensional reduction to $(1+1)$ Sine-Gordon model, appropriate in a strong magnetic field; and iii) holographic QCD (Sakai-Sugimoto model), appropriate at strong coupling. We also briefly discuss the phenomenological implications of the CMW for heavy ion collisions.

Chiral Magnetic Wave

TL;DR

This work demonstrates that triangle anomalies in magnetized relativistic plasmas generate a new gapless collective mode, the Chiral Magnetic Wave (CMW), coupling electric and chiral charge density waves and propagating along the magnetic field. It derives and cross-validates the CMW across three frameworks: relativistic magnetohydrodynamics, strong-field dimensional reduction to a 1+1D Sine-Gordon description, and holographic QCD via the Sakai–Sugimoto model, revealing a nonperturbative, field-dependent wave velocity that approaches the speed of light at large . By incorporating dynamical electromagnetism, the study shows how CMW mixes with plasmons, altering plasmon dispersions and yielding Schwinger-type photon masses in strong fields. The results have potential implications for heavy-ion collision phenomenology, including reaction-plane dependent charge fluctuations, and establish a robust, multi-method confirmation of the CMW across weak and strong coupling regimes.

Abstract

We consider a relativistic plasma containing charged chiral fermions in an external magnetic field, e.g a chirally symmetric quark-gluon plasma created in relativistic heavy ion collisions. We show that triangle anomalies imply the existence of a new type of collective gapless excitation in this system that stems from the coupling between the density waves of the electric and chiral charges; we call it "the Chiral Magnetic Wave" (CMW). The CMW exists even in a neutral plasma, i.e. in the absence of the axial and vector chemical potentials. We demonstrate the existence of CMW and study its properties using three different approaches: i) relativistic magnetohydrodynamics; ii) dimensional reduction to Sine-Gordon model, appropriate in a strong magnetic field; and iii) holographic QCD (Sakai-Sugimoto model), appropriate at strong coupling. We also briefly discuss the phenomenological implications of the CMW for heavy ion collisions.

Paper Structure

This paper contains 6 sections, 101 equations, 4 figures.

Figures (4)

  • Figure 1: Anomalous triangle diagrams of chiral magnetic waves for (a) abelian and (b) non-abelian flavor symmetries in the presence of external magnetic field $B$. The quark lines are dressed propagators including the background magnetic field.
  • Figure 2: A schematic picture of $D8-\overline{D8}$ branes in deconfined phase of the Sakai-Sugimoto model.
  • Figure 3: Numerical result for $v_\chi$ in the Sakai-Sugimoto model with $T=150$ MeV(dotted), $T=200$ MeV(plain), and $T=250$ MeV(dashed).
  • Figure 4: Numerical result for $D_L$ in the Sakai-Sugimoto model with $T=150$ MeV(dotted), $T=200$ MeV(plain), and $T=250$ MeV(dashed).