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Acoustic phonons in a magnetized vacuum? First-principle lattice results on the mass spectrum of the electroweak model in a strong magnetic field

M. N. Chernodub1,2, V. A. Goy3,4, and A. V. Molochkov1,3,5

Phys. Rev. D 113, 074508 – Published 14 April, 2026

DOI: https://doi.org/10.1103/b4cm-y63c

Abstract

We use numerical Monte Carlo simulations to determine the mass spectrum of the bosonic sector of the electroweak model in an external magnetic field of the electroweak-scale strength (1020T) at zero temperature. It is known that as the magnetic field gets stronger, the electroweak vacuum undergoes two consecutive crossover-type transitions, passing from (i) the conventional symmetry-broken homogeneous phase to (ii) an intermediate inhomogeneous vortex phase characterized by a (superconducting) condensate of electrically charged W bosons and then to (iii) a homogeneous phase with a restored electroweak symmetry. We show that the spin component of the W boson aligned with the direction of the magnetic field is the lightest excitation in all three phases. Its mass continuously decreases in the low-field broken phase and becomes very small in the intermediate phase. We argue that this nearly massless excitation corresponds to a Goldstone acoustic phonon mode associated with vibrations of the lattice of electroweak vortices. In the high-field symmetry-restored phase, where the vortices disappear, the lightest W mass rises again. Neither Higgs nor Z boson masses vanish across all studied phases and crossover transitions.

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Phase Structure of Electroweak Vacuum in a Strong Magnetic Field: The Lattice Results

M. N. Chernodub, V. A. Goy, and A. V. Molochkov
Phys. Rev. Lett. 130, 111802 (2023)

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