Smallness of neutrino masses and leptogenesis in 331 composite Higgs model

We consider 331 composite Higgs model (CHM3) in which the Lagrangian of the strongly coupled sector is invariant with respect to global SU (3) C × SU (3) × U (1) 6 symmetry that can originate from SU (6) subgroup of E 6 and contains the gauge group of the standard model (SM) as a subgroup. The breakdown of the approximate SU (3) × U (1) 6 symmetry down to SU (2) W × U (1) Y subgroup around the scale f ∼ 10 TeV results in a set of pseudo–Nambu–Goldstone bosons (pNGBs) that, in particular, involves Higgs doublet. The generation of the masses of the SM fermions in the CHM3 is discussed. We argue that approximate U (1) L and discrete Z 2 symmetries may give rise to tiny masses of the left–handed neutrinos and several composite fermions with masses 1 − 2 TeV . The lepton and baryon asymmetries can be generated within the CHM3 via the out–of equilibrium decays of extra Majorana particle into the Higgs doublet and these composite fermions.

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Publication Details

Journal
Physics Letters B
Published
2026-01-23
DOI
https://doi.org/10.1016/j.physletb.2026.140210
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
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article

Smallness of neutrino masses and leptogenesis in 331 composite Higgs model

R. Nevzorov
Physics Letters B
Particle physics theoretical and experimental studies
article

Smallness of neutrino masses and leptogenesis in 331 composite Higgs model

R. Nevzorov
article en

Abstract

We consider 331 composite Higgs model (CHM3) in which the Lagrangian of the strongly coupled sector is invariant with respect to global SU (3) C × SU (3) × U (1) 6 symmetry that can originate from SU (6) subgroup of E 6 and contains the gauge group of the standard model (SM) as a subgroup. The breakdown of the approximate SU (3) × U (1) 6 symmetry down to SU (2) W × U (1) Y subgroup around the scale f ∼ 10 TeV results in a set of pseudo–Nambu–Goldstone bosons (pNGBs) that, in particular, involves Higgs doublet. The generation of the masses of the SM fermions in the CHM3 is discussed. We argue that approximate U (1) L and discrete Z 2 symmetries may give rise to tiny masses of the left–handed neutrinos and several composite fermions with masses 1 − 2 TeV . The lepton and baryon asymmetries can be generated within the CHM3 via the out–of equilibrium decays of extra Majorana particle into the Higgs doublet and these composite fermions.

Physics Letters BVol. 874
P.N. Lebedev Physical Institute of the Russian Academy of Sciences (RU)
Openalex Percentile: Top 76%
Particle physics theoretical and experimental studies
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