Dirac-phase thermal leptogenesis in the extended type-I seesaw model

被引:35
|
作者
Dolan, Matthew J. [1 ]
Dutka, Tomasz P. [1 ]
Volkas, Raymond R. [1 ]
机构
[1] Univ Melbourne, ARC Ctr Excellence Particle Phys Terascale, Sch Phys, Melbourne, Vic 3010, Australia
来源
JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS | 2018年 / 06期
基金
澳大利亚研究理事会;
关键词
baryon asymmetry; leptogenesis; neutrino theory; particle physics; cosmology connection; LOW-SCALE LEPTOGENESIS; LEFT-RIGHT SYMMETRY; NEUTRINO MASS; LEPTON-NUMBER; FLAVOR VIOLATION; BARYOGENESIS; BARYON; NONCONSERVATION; DECAYS; GAMMA;
D O I
10.1088/1475-7516/2018/06/012
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Motivated by the fact that delta(CP), the Dirac phase in the PMNS matrix, is the only CP-violating parameter in the leptonic sector that can be measured in neutrino oscillation experiments, we examine the possibility that it is the dominant source of CP violation for leptogenesis caused by the out-of-equilibrium decays of heavy singlet fermions. We do so within a low-scale extended type-I seesaw model, featuring two Standard Model singlet fermions per family, in which lepton number is approximately conserved such that the heavy singlet neutrinos are pseudo-Dirac. We find that this produces a predictive model of leptogenesis. Our results show that for low-scale thermal leptogenesis, a pure inverse-seesaw scenario fails to produce the required asymmetry, even accounting for resonance effects, because wash-out processes are too efficient. Dirac-phase leptogenesis is, however, possible when the linear seesaw term is switched on, with the aid of the resonance contributions naturally present in the model. Degenerate and hierarchical spectra are considered both can achieve (Scpleptogenesis, although the latter is more constrained. Finally, although unable to probe the parameter space of Dirac-phase leptogenesis, the contributions to unitarity violation of the PMNS matrix, collider constraints and charged-lepton flavour-violating processes are calculated and we further estimate the impact of the future experiments MEG-II and COMET for such models.
引用
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页数:39
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