Magnetic field evolution in feedback-dominated galaxies

arXiv:2610.17216 · astro-ph.GA · Submitted 2026-10-12 · Read on arXiv

astro-ph.GA

Submitted: 2026-10-12

Updated: 2026-10-12

Comments: 17 pages, of which 12 are the main text, with 8 figures and 1 table. Submitted to MNRAS. Comments welcome!

Project page: http://fire.northwestern.edu

License: http://creativecommons.org/licenses/by/4.0/

The gist: Over the last decade, magnetic fields (B-fields) have become a common ingredient in galaxy formation simulations.

Abstract

Over the last decade, magnetic fields (B-fields) have become a common ingredient in galaxy formation simulations. Although seemingly unimportant in matching observational constraints such as the M*-M halo relations, the B-field influences the circumgalactic medium (CGM) gas and determines cosmic ray (CR) propagation, making it an indispensable non-thermal component. Nevertheless, the intricate physics of B-fields, particularly how they evolve to the observed μ G-level field, remains largely elusive. In this work, we systematically address the evolution of B-fields over cosmic time using the FIRE-2 (Feedback In Realistic Environments) magnetohydrodynamics (MHD) simulations. We present results for both Milky Way (MW)-mass and dwarf galaxies, with and without CRs. We find that CRs have little impact on B-field properties, while the halo mass controls the saturated B-field strength at z about 0. However, all runs reach a halo-independent magnetic-to-turbulent ratio of f B about 1-10%, though the methods used to measure turbulence could affect this value. We identify a three-stage evolutionary course for the B-field in tandem with galaxy formation: i. expansion, ii. amplification, and iii. saturation. The feature is universal, though the timings depend on the initial location and star formation history of the gas. Flux-freezing is the predominant driver for the first and last stages, exhibiting power relations B about ρ 2/3 and ρ 1/2, although the latter could also be explained by dynamical and energetic equilibria. The intermediate amplification stage, potentially driven by ``dynamos'', is fuelled by structure formation, feedback, and gas turbulence. We conjecture a numerically triggered, turbulence-driven amplification process to explain this phenomenon.

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