Inverse electroweak baryogenesis

A bstract We propose a mechanism for baryogenesis in which the baryon asymmetry is generated as an equilibrium response of weak sphalerons in a region where electroweak sphaleron transitions remain unsuppressed, h / T ≲ 1. A nonzero equilibrium baryon density arises in the presence of an approximately conserved global charge, carried either by new states with nonzero hypercharge, or by Standard Model fields themselves. The required global charge asymmetry is generated during a phase transition that changes the strength of electroweak symmetry breaking, but need not coincide with the final electroweak phase transition. In particular, the mechanism can operate during an inverse electroweak phase transition, where baryon number is produced behind the advancing wall, in contrast to conventional electroweak baryogenesis. Because baryon production is decoupled from a direct first-order electroweak phase transition, the scenario can be realized at parametrically higher temperatures than standard electroweak baryogenesis, thereby weakening current experimental constraints. This framework provides a qualitatively distinct route to electroweak baryogenesis, with different parametric dependence, phase-transition dynamics, and phenomenological signatures.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-09-16
DOI
https://doi.org/10.1007/jhep09(2026)184
Primary Topic
Earthquake Detection and Analysis
Type
article
Field-Weighted Citation Impact
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article

Inverse electroweak baryogenesis

Oleksii Matsedonskyi, Jacopo Azzola, Andreas Weiler
Journal of High Energy Physics
Earthquake Detection and Analysis
article

Inverse electroweak baryogenesis

Oleksii Matsedonskyi, Jacopo Azzola, Andreas Weiler
article en

Abstract

A bstract We propose a mechanism for baryogenesis in which the baryon asymmetry is generated as an equilibrium response of weak sphalerons in a region where electroweak sphaleron transitions remain unsuppressed, h / T ≲ 1. A nonzero equilibrium baryon density arises in the presence of an approximately conserved global charge, carried either by new states with nonzero hypercharge, or by Standard Model fields themselves. The required global charge asymmetry is generated during a phase transition that changes the strength of electroweak symmetry breaking, but need not coincide with the final electroweak phase transition. In particular, the mechanism can operate during an inverse electroweak phase transition, where baryon number is produced behind the advancing wall, in contrast to conventional electroweak baryogenesis. Because baryon production is decoupled from a direct first-order electroweak phase transition, the scenario can be realized at parametrically higher temperatures than standard electroweak baryogenesis, thereby weakening current experimental constraints. This framework provides a qualitatively distinct route to electroweak baryogenesis, with different parametric dependence, phase-transition dynamics, and phenomenological signatures.

Journal of High Energy PhysicsVol. 2026(9)
Technical University of Munich (DE)
Openalex Percentile: Top 79%
Earthquake Detection and Analysis
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