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Neutrino masses and the baryon asymmetry
High Energy Physics - Phenomenology · Submitted 17 Jul 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim For hierarchical neutrino masses, with $B-L$ broken at the unification scale $\Lambda_{GUT}\sim 10^{16} $GeV, the observed baryon asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained by the decay of heavy Majorana neutrinos.
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The abstract, sentence by sentence
Due to sphaleron processes in the high-temperature symmetric phase of the standard model the cosmological baryon asymmetry is related to neutrino properties. For hierarchical neutrino masses, with $B-L$ broken at the unification scale $\Lambda_{GUT}\sim 10^{16} $GeV, the observed baryon asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained by the decay of heavy Majorana neutrinos. We illustrate this mechanism with two models of neutrino masses, consistent with the solar and atmospheric neutrino anomalies, which are based on the two symmetry groups $SU(5)\times U(1)_F$ and $SU(3)_c\times SU(3)_L\times SU(3)_R\times U(1)_F$. We also review related cosmological bounds on Majorana neutrino masses and the use of Boltzmann equations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Due to sphaleron processes in the high-temperature symmetric phase of the standard model the cosmological baryon asymmetry is related to neutrino properties. | background 1.00 | 0.07 | 0.20 | asserted 1.00 |
| s1 | For hierarchical neutrino masses, with $B-L$ broken at the unification scale $\Lambda_{GUT}\sim 10^{16} $GeV, the observed baryon asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained by the decay of heavy Majorana neutrinos. | result 0.43 | 0.18 | 0.65 | asserted 0.75 |
| s2 | We illustrate this mechanism with two models of neutrino masses, consistent with the solar and atmospheric neutrino anomalies, which are based on the two symmetry groups $SU(5)\times U(1)_F$ and $SU(3)_c\times SU(3)_L\times SU(3)_R\times U(1)_F$. | contribution 0.72 | 0.86 | 0.10 | asserted 0.96 |
| s3 | We also review related cosmological bounds on Majorana neutrino masses and the use of Boltzmann equations. | contribution 0.67 | 0.36 | 0.03 | asserted 0.69 |
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The paper
Original abstract
Due to sphaleron processes in the high-temperature symmetric phase of the standard model the cosmological baryon asymmetry is related to neutrino properties. For hierarchical neutrino masses, with $B-L$ broken at the unification scale $\Lambda_{GUT}\sim 10^{16} $GeV, the observed baryon asymmetry $n_B/s \sim 10^{-10}$ can be naturally explained by the decay of heavy Majorana neutrinos. We illustrate this mechanism with two models of neutrino masses, consistent with the solar and atmospheric neutrino anomalies, which are based on the two symmetry groups $SU(5)\times U(1)_F$ and $SU(3)_c\times SU(3)_L\times SU(3)_R\times U(1)_F$. We also review related cosmological bounds on Majorana neutrino masses and the use of Boltzmann equations.
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References
How the literature uses it
8 arXiv papers cite this in 10 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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For hierarchical neutrino masses, with B-L broken at the unification scale $\Lambda_{GUT} \sim 10^{16}$ GeV, the observed baryon asymmetry $n_B/s \sim 10^{-10}$ is naturally explained by the decay of heavy Majorana neutrinos.
Papers citing it · 7 sentences without a confident label
Cites it as background 3 papers
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This well-known obstacle has triggered many attempts in the popular seesaw-based leptogenesis [ref] to source the baryon asymmetry uniquely from the CP-violating phase in the PMNS matrix (we call this connection the unique phase source hereafter), where assumptions and/or parametrizations of the neutrino Dirac-Yukawa structure are generically made, such as the widely used Casas-Ibarra parametrization [ref] ; see also some earlier and recent considerations [ref] .
Baryogenesis from Hierarchical Dirac Neutrinos · Introduction · 0.87
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A well-studied realization, “thermal leptogenesis,” invokes hierarchical heavy neutrino masses $M_1 ≪M_i>1$ [ref] .
A Model of Annihilogenesis · Introduction · 0.95
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A generic way is to invoke some assumptions or parametrizations of the lepton Yukawa structures, as widely considered in Refs. [ref] .
Next-to-tribimaximal mixing against CP violation and baryon asymmetry signs · Introduction · 0.85
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