Neutrino mass, dark matter and anomalous magnetic moment of muon in a U(1)Lμ-LT model

被引:0
|
作者
Biswas, Anirban [1 ]
Choubey, Sandhya [1 ,2 ]
Khan, Sarif [1 ]
机构
[1] Harish Chandra Res Inst, Chhatnag Rd, Allahabad 211019, Uttar Pradesh, India
[2] AlbaNova Univ Ctr, KTH Royal Inst Technol, Sch Engn Sci, Dept Theoret Phys, S-10691 Stockholm, Sweden
来源
关键词
Neutrino Physics; Beyond Standard Model; Cosmology of Theories beyond the SM; REACTOR ANTINEUTRINO DISAPPEARANCE; TAU SYMMETRY; FLAVOR SYMMETRY; GALACTIC-CENTER; CP VIOLATION; EMISSION; PARTICLES; BREAKING; MIXINGS; MATRIX;
D O I
10.1007/JHEP09(2016)147
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
The observation of neutrino masses, mixing and the existence of dark matter are amongst the most important signatures of physics beyond the Standard Model (SM). In this paper, we propose to extend the SM by a local L-mu-L-T gauge symmetry, two additional complex scalars and three right-handed neutrinos. The L-mu-L-T gauge symmetry is broken spontaneously when one of the scalars acquires a vacuum expectation value. The L-mu-L-T gauge symmetry is known to be anomaly free and can explain the beyond SM measurement of the anomalous muon (g - 2) through additional contribution arising from the extra Z(mu T) mediated diagram. Small neutrino masses are explained naturally through the Type-I seesaw mechanism, while the mixing angles are predicted to be in their observed ranges due to the broken L-mu-L-T symmetry. The second complex scalar is shown to be stable and becomes the dark matter candidate in our model. We show that while the Z(mu T) portal is ineffective for the parameters needed to explain the anomalous muon (g 2) data, the correct dark matter relic abundance can easily be obtained from annihilation through the Higgs portal. Annihilation of the scalar dark matter in our model can also explain the Galactic Centre gamma ray excess observed by Fermi-LAT. We show the predictions of our model for future direct detection experiments and neutrino oscillation experiments.
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页数:31
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