2022
DOI: 10.1007/jhep08(2022)078
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Annihilogenesis

Abstract: We investigate a novel interplay between the decay and annihilation of a particle whose mass undergoes a large shift during a first order phase transition, leading to the particles becoming trapped in the false vacuum and enhancing their annihilation rates as the bubbles of true vacuum expand. This opens up a large region of the parameter space where annihilations can be important. We apply this scenario to baryogenesis, where we find that annihilations can be enhanced enough to generate the required baryon as… Show more

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Cited by 10 publications
(5 citation statements)
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“…2 One might concern that in case of M 1 /T p 1 the RHNs do not have sufficient energy to cross the wall, as the average kinetic energy of ν R is O(T p ). Were that true, most of the RHNs will be trapped in the old vacuum [27][28][29][30][31], and only a tiny fraction of them can be "filtered" to the new vacuum [32][33][34][35], resulting in a much suppressed ν R number density in the φ = 0 phase, and the resultant BAU is also negligible, as pointed out in [26,36]. This issue, however, can be solved, provided that the bubbles are expanding in an ultrarelativistic velocity, i.e.…”
Section: Jhep09(2022)052mentioning
confidence: 99%
“…2 One might concern that in case of M 1 /T p 1 the RHNs do not have sufficient energy to cross the wall, as the average kinetic energy of ν R is O(T p ). Were that true, most of the RHNs will be trapped in the old vacuum [27][28][29][30][31], and only a tiny fraction of them can be "filtered" to the new vacuum [32][33][34][35], resulting in a much suppressed ν R number density in the φ = 0 phase, and the resultant BAU is also negligible, as pointed out in [26,36]. This issue, however, can be solved, provided that the bubbles are expanding in an ultrarelativistic velocity, i.e.…”
Section: Jhep09(2022)052mentioning
confidence: 99%
“…See refs [52][53][54]. for other baryogenesis and dark matter mechanisms involving particle trapping, and refs [55][56][57][58][59][60][61][62][63][64][65].…”
mentioning
confidence: 99%
“…However, for the false vacuum remnants to be sufficiently dense to collapse into PBHs, we have to address an important issue: how to prevent the trapped fermions from disappearing through χ χ → φ, φφ, etc, and eventually to the SM particles in the thermal bath? Such annihilations are inevitably enhanced when the remnants shrink, reducing the fermion number density greatly [165,166] and consequently destroying any possibility of collapse into PBHs. To have PBHs formed, there are two typical scenarios: I.…”
Section: Jcap06(2023)008mentioning
confidence: 99%