论文标题

冻结狄拉克中性生成:热麻血CP不对称

Freeze-in Dirac neutrinogenesis: thermal leptonic CP asymmetry

论文作者

Li, Shao-Ping, Li, Xin-Qiang, Yan, Xin-Shuai, Yang, Ya-Dong

论文摘要

我们提出了狄拉克中性生成的冻结实现,其中产生Lepton-number不对称的腐烂粒子处于热平衡状态。由于右撇子中微子是非热中的,因此积累了Lepton-number不对称性,并通过快速的Sphaleron跃迁部分转化为BARYON非对称性。可以通过从Lepton-Doublet扇区的波函数校正来实现必要的CP侵略条件,该阶段在大多数基于瘦素的设置中都被忽略了。此外,这种条件需要一个首选的风味基础,即带电的lepton和中微子Yukawa矩阵都是非二角形的。为了保护这种合适的Yukawa结构免受电气量规对称性破裂之前风味空间的基础转换,我们可以诉诸于旨在破译非平凡Yukawa结构的大量模型建筑物。 Interestingly, based on the well-known tri-bimaximal mixing with a minimal correction from the charged-lepton or neutrino sector, we find that a simultaneous explanation of the baryon-number asymmetry in the Universe and the low-energy neutrino oscillation observables can be attributed to the mixing angle and the CP-violating phase introduced in the minimal correction.

We present a freeze-in realization of the Dirac neutrinogenesis in which the decaying particle that generates the lepton-number asymmetry is in thermal equilibrium. As the right-handed Dirac neutrinos are produced non-thermally, the lepton-number asymmetry is accumulated and partially converted to the baryon-number asymmetry via the rapid sphaleron transitions. The necessary CP-violating condition can be fulfilled by a purely thermal kinetic phase from the wavefunction correction in the lepton-doublet sector, which has been neglected in most leptogenesis-based setup. Furthermore, this condition necessitates a preferred flavor basis in which both the charged-lepton and neutrino Yukawa matrices are non-diagonal. To protect such a proper Yukawa structure from the basis transformations in flavor space prior to the electroweak gauge symmetry breaking, we can resort to a plethora of model buildings aimed at deciphering the non-trivial Yukawa structures. Interestingly, based on the well-known tri-bimaximal mixing with a minimal correction from the charged-lepton or neutrino sector, we find that a simultaneous explanation of the baryon-number asymmetry in the Universe and the low-energy neutrino oscillation observables can be attributed to the mixing angle and the CP-violating phase introduced in the minimal correction.

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