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arxiv: 1612.00032 · v2 · pith:EKPTD7I2new · submitted 2016-11-30 · ✦ hep-ph · astro-ph.HE· nucl-th

Energy Conservation and the Chiral Magnetic Effect

classification ✦ hep-ph astro-ph.HEnucl-th
keywords plasmachiralmagneticenergypotentialstateconservationeffect
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We analyze the chiral magnetic effect in a homogeneous neutral plasma from the point of view of energy conservation, and construct an effective potential for the growth of maximally helical perturbations of the electromagnetic field. We show that a negative curvature at the origin of the potential, indicating instability of the plasma, is induced by a chiral asymmetry in electron Fermi energy, as opposed to number density, while the potential grows at large field value. It follows that the ground state for a plasma has zero magnetic helicity; a nonzero electron mass will allow an excited state of a plasma with nonzero helicity to relax to that ground state quickly. We conclude that a chiral plasma instability triggered by weak interactions is not a viable mechanism for explaining magnetic fields in stars except possibly when dynamics drives the system far from equilibrium.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Chiral effects and Joule heating in hot and dense matter

    hep-ph 2025-09 unverdicted novelty 6.0

    Higher temperatures enable chiral plasma instability to grow magnetic fields from modest chiral chemical potentials, while CME from density fluctuations produces rapid Joule heating reaching QCD-scale energies in mill...

  2. Magnetar field dynamics driven by chiral anomalies without magnetic helicity

    astro-ph.HE 2026-05 unverdicted novelty 5.0

    Chiral magnetic effect generates magnetar-strength dipoles independently of initial net helicity via localized structures on decade timescales.

  3. Plasma heating during the chiral plasma instability

    hep-ph 2026-05 unverdicted novelty 5.0

    During chiral plasma instability, excess energy from chiral asymmetry heats the plasma with δT ~ μ5²/T instead of fully building the helical magnetic field.