×
近期发现有不法分子冒充我刊与作者联系,借此进行欺诈等不法行为,请广大作者加以鉴别,如遇诈骗行为,请第一时间与我刊编辑部联系确认(《中国物理C》(英文)编辑部电话:010-88235947,010-88236950),并作报警处理。
本刊再次郑重声明:
(1)本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137
(2)本刊采编系统作者中心是投稿的唯一路径,该系统为ScholarOne远程稿件采编系统,仅在本刊投稿网网址(https://mc03.manuscriptcentral.com/cpc)设有登录入口。本刊不接受其他方式的投稿,如打印稿投稿、E-mail信箱投稿等,若以此种方式接收投稿均为假冒。
(3)所有投稿均需经过严格的同行评议、编辑加工后方可发表,本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿,并收取发表费用,均为假冒。
                  
《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.
      PCAS:
  • 加载中
  • [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)
  • 加载中

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
Milestone
Received: 2016-07-14
Revised: 2016-11-23
Fund

    This work is supported by DST-Inspire Fellowship division-IF130927

Article Metric

Article Views(1513)
PDF Downloads(50)
Cited by(0)
Policy on re-use
To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

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.

    HTML

Reference (23)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return