Leptogenesis in the presence of density perturbations

We point out a new effect on the freeze-out process of heavy particles induced by density perturbations in the early Universe, which we call “acoustically driven freeze-out.” This beyond-linear effect is caused by the exponential decoupling of heavy particles from the thermal bath in the presence of density perturbations, and already at moderately large values <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>δ</a:mi><a:mi>T</a:mi><a:mo>/</a:mo><a:mover accent="true"><a:mi>T</a:mi><a:mo stretchy="false">¯</a:mo></a:mover><a:mo>=</a:mo><a:mi mathvariant="script">O</a:mi><a:mo stretchy="false">(</a:mo><a:msup><a:mn>10</a:mn><a:mrow><a:mo>−</a:mo><a:mn>2</a:mn></a:mrow></a:msup><a:mo stretchy="false">)</a:mo></a:math>, it cannot be captured by linear perturbation theory. We illustrate this effect with leptogenesis taking the decay and inverse decay of heavy neutrinos into account and discuss its phenomenological implications. We found that perturbations always enhance the (spatially averaged) values of the final lepton asymmetry, and as a result, constraints on the mass of heavy neutrinos are found to be relaxed in the presence of perturbations.

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Journal
Physical review. D/Physical review. D.
Published
2025-05-20
DOI
https://doi.org/10.1103/s7dp-8f59
Primary Topic
Fractal and DNA sequence analysis
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article
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article

Leptogenesis in the presence of density perturbations

Karl J. Friston
Physical review. D/Physical review. D.
Fractal and DNA sequence analysis
article

Leptogenesis in the presence of density perturbations

Karl J. Friston
article en

Abstract

We point out a new effect on the freeze-out process of heavy particles induced by density perturbations in the early Universe, which we call “acoustically driven freeze-out.” This beyond-linear effect is caused by the exponential decoupling of heavy particles from the thermal bath in the presence of density perturbations, and already at moderately large values <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mi>δ</a:mi><a:mi>T</a:mi><a:mo>/</a:mo><a:mover accent="true"><a:mi>T</a:mi><a:mo stretchy="false">¯</a:mo></a:mover><a:mo>=</a:mo><a:mi mathvariant="script">O</a:mi><a:mo stretchy="false">(</a:mo><a:msup><a:mn>10</a:mn><a:mrow><a:mo>−</a:mo><a:mn>2</a:mn></a:mrow></a:msup><a:mo stretchy="false">)</a:mo></a:math>, it cannot be captured by linear perturbation theory. We illustrate this effect with leptogenesis taking the decay and inverse decay of heavy neutrinos into account and discuss its phenomenological implications. We found that perturbations always enhance the (spatially averaged) values of the final lepton asymmetry, and as a result, constraints on the mass of heavy neutrinos are found to be relaxed in the presence of perturbations.

Physical review. D/Physical review. D.Vol. 111(11)
Kobe University (JP), The University of Tokyo (JP)
Climate action
Openalex Percentile: Top 90%
Fractal and DNA sequence analysis
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Leptogenesis in the presence of density perturbations — Karl J. Friston · Physical review. D/Physical review. D. (2025) | TGRS Research Map | TGRS