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《中国物理C》(英文)编辑部
2024年10月30日

Implications of fermionic dark matter on recent neutrino oscillation data

  • We investigate flavor phenomenology and dark matter in the context of the scotogenic model. In this model, the neutrino masses are generated through radiative corrections at the one-loop level. Considering the neutrino mixing matrix to be of tri-bimaximal form with additional perturbations to accommodate the recently observed non-zero value of the reactor mixing angle θ13, we obtain the relation between various neutrino oscillation parameters and the model parameters. Working in a degenerate heavy neutrino mass spectrum, we obtain light neutrino masses obeying the normal hierarchy and also study the relic abundance of fermionic dark matter candidates, including coannihilation effects. A viable parameter space is thus obtained, consistent with neutrino oscillation data, relic abundance and various lepton flavor violating decays such as lα→lβγ and lα→3lβ.
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  • [1] P. Minkowski, Phys. Lett. B, 67:421 (1977); R. N. Mohapatra and G. Senjanovic, Phys. Rev. Lett., 44:912 (1980); M. Gell-Mann, P. Ramond, and R. Slansky (1980), print-80-0576 (CERN); J. Schechter and J. W. F. Valle, Phys. Rev. D, 22:2227 (1980)
    [2] R. N. Mohapatra and G. Senjanovic, Phys. Rev. D, 23:165 (1981); G. Lazarides, Q. Shafi, and C. Wetterich, Nucl. Phys. B, 181:287 (1981); C. Wetterich, Nucl. Phys. B, 187:343 (1981); B. Brahmachari and R. N. Mohapatra, Phys. Rev. D, 58:015001 (1998); S. Antusch and S. F. King, Phys. Lett. B, 597:199 (2004); R. N. Mohapatra, Nucl. Phys. Proc. suppl., 138:257 (2005)
    [3] R. Foot, H. Lew, X. G. He et al, Z. Phys. C, 44:441 (1989)
    [4] E. Ma, Phys. Rev. D, 73:077301 (2006), arXiv:hepph/0601225
    [5] B. Pontecorvo, Sov. Phys. JETP, 7:172 (1958); Z. Maki, M. Nakagawa, and S. Sakata, Prog. Theor. Phys., 28:870 (1962)
    [6] F. P. An et al (DAYA-BAY Collaboration), Phys. Rev. Lett., 108:171803 (2012), arXiv:1203.1669
    [7] F. P. An et al (DAYA-BAY Collaboration), Chin. Phys. C, 37:011001 (2013), arXiv:1210.6327
    [8] J. K. Ahn et al (RENO Collaboration), Phys. Rev. Lett., 108:191802 (2012), arXiv:1204.0626
    [9] K. Abe et al (T2K Collaboration), Phys. Rev. D, 88:032002 (2013), arXiv:1304.0841
    [10] D. Forero, M. Tortela, and J. Valle, Phys. Rev. D, 90:093006 (2014), arXiv:1405.7540
    [11] P. A. R. Ade et al (Planck Collaboration), Astron. Astrophys., 571:A1 (2014), arXiv:1303.5062
    [12] L. Lepoz Honorez, E.Nezri, J. F. Oliver et al, JCAP, 02:28 (2007), arXiv:hep-ph/0612275
    [13] R. Barbieri, L. E. Hall, and V. S. Rychkov, Phys. Rev. D, 74:015007 (2006), arXiv:hep-ph/0603188
    [14] M. Gustafsson, PoS CHARGED, 2010:030 (2010), arXiv:1106.1719
    [15] Daijiro Suematsu, Takashi Toma, Tetsuro Yoshida, Phys. Rev. D, 79:093004 (2009), arXiv:0903.0287
    [16] D. Schmidt, T Schwetz, and T. Toma, Phys. Rev. D, 85:073009 (2012), arXiv:1201.0906
    [17] T. Toma and A. Vicente, JHEP, 01:160 (2014), arXiv:1312.2840
    [18] A. Vicente, C E. Yaguna, JHEP, 02:144 (2015), arXiv:1412.2545
    [19] G. Altarelli, F. Ferugilo, Rev. Mod. Phys., 82:2701 (2010); G. Altarelli, F. Ferugilo, L. Merlo, and E. Stamou, JHEP, 08:021 (2012), arXiv:1205.4670; S. F. King and C. Luhn, Rept. Prog. Phys., 76:056201 (2013), arXiv:1301.1340; S. F. King, A. Merle, S. Morisi et al, New Journ. Phys., 16:045018 (2014); H. Isimori et al, Prog. Theor. Phys. Suppl., 183:1 (2010)
    [20] P. F. Harrison, D. H. Perkins, and W.G. Scott, Phys. Lett. B, 458:79 (1999); Phys. Lett. B, 530:167 (2002); Z. Z. Xing, Phys. Lett. B, 533:85 (2002); P. F. Harrison and W. G. Scott, Phys. Lett. B, 535:163 (2002); Phys. Lett. B, 557:76 (2003); X.-G. He and A. Zee, Phys. Lett. B, 560:87 (2003); L. Wolfenstein, Phys. Rev. D, 18:958 (1978); Y. Yamanaka, H. Sugawara, and S. Pakvasa, Phys. Rev. D, 25:1895 (1982); D, 29:2135(E) (1984); N. Li and B.-Q. Ma, Phys. Rev. D, 71:017302 (2005), arXiv:hep-ph/0412126
    [21] M. Sruthilaya, C. Soumya, K.N. Deepthi et al, New J. Phys., 17:083028 (2015), arXiv:1408.4392
    [22] K. Griest and D. Seckel, Phys. Rev. D, 43:3191 (1991)
    [23] K. A. Olive et al, Particle Data Group Collaboration, Chin. Phys. C, 38:090001 (2014)
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Get Citation
Shivaramakrishna Singirala. Implications of fermionic dark matter on recent neutrino oscillation data[J]. Chinese Physics C, 2017, 41(4): 043102. doi: 10.1088/1674-1137/41/4/043102
Shivaramakrishna Singirala. Implications of fermionic dark matter on recent neutrino oscillation data[J]. Chinese Physics C, 2017, 41(4): 043102.  doi: 10.1088/1674-1137/41/4/043102 shu
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Received: 2016-07-14
Revised: 2016-11-23
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    This work is supported by DST-Inspire Fellowship division-IF130927

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Implications of fermionic dark matter on recent neutrino oscillation data

  • 1. School of Physics, University of Hyderabad, Hyderabad-500046, India
Fund Project:  This work is supported by DST-Inspire Fellowship division-IF130927

Abstract: We investigate flavor phenomenology and dark matter in the context of the scotogenic model. In this model, the neutrino masses are generated through radiative corrections at the one-loop level. Considering the neutrino mixing matrix to be of tri-bimaximal form with additional perturbations to accommodate the recently observed non-zero value of the reactor mixing angle θ13, we obtain the relation between various neutrino oscillation parameters and the model parameters. Working in a degenerate heavy neutrino mass spectrum, we obtain light neutrino masses obeying the normal hierarchy and also study the relic abundance of fermionic dark matter candidates, including coannihilation effects. A viable parameter space is thus obtained, consistent with neutrino oscillation data, relic abundance and various lepton flavor violating decays such as lα→lβγ and lα→3lβ.

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