A model with flavor-dependent gauged U(1)B-L1&times;U(1)B-L2-L3 symmetry

Linping Mu; Hiroshi Okada; Chao-Qiang Geng

doi:10.1088/1674-1137/42/12/123106

Chinese Physics C> 2018, Vol. 42> Issue(12) : 123106 DOI: 10.1088/1674-1137/42/12/123106

A model with flavor-dependent gauged U(1)_B-L₁×U(1)_B-L₂-L₃ symmetry

Linping Mu ^1,, ,
Hiroshi Okada ^2,3,, ,
Chao-Qiang Geng ^1,2,4,,

1.
School of Physics and Information Engineering, Shanxi Normal University, Linfen 041004
2.
Physics Division, National Center for Theoretical Sciences, Hsinchu, Taipei 300
3.
Asia Pacific Center for Theoretical Physics, Pohang, Geyoengbuk 790-784
4.
School of Physics and Information Engineering, Shanxi Normal University, Linfen 041004
5.
Physics Division, National Center for Theoretical Sciences, Hsinchu, Taipei 300
6.
Department of Physics, National Tsing Hua University, Hsinchu, Taipei 300

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Abstract：
We propose a new model with flavor-dependent gauged U(1)_B-L₁×U(1)_B-L₂-L₃ symmetry in addition to the flavor-blind symmetry in the Standard Model. The model contains three right-handed neutrinos to cancel gauge anomalies and several Higgs bosons to construct the measured fermion masses. We show the generic features of the model and explore its phenomenology. In particular, we discuss the current bounds on the extra gauge bosons from the K and B meson mixings as well as the LEP and LHC data, and focus on their contributions to the lepton flavor violating processes of l_i+1→l_iγ (i=1,2).
- flavor-dependent gauged Abelian symmetries ,
- model building ,
- numerical analysis of gauge boson masses and coupling

References

[1]	H. Fritzsch and P. Minkowski, Annals Phys., 93:193(1975), doi:10.1016/0003-4916(75)90211-0
[2]	P. Ko, T. Nomura, and H. Okada, Phys. Rev. D, 95(11):111701(2017), doi:10.1103/PhysRevD.95.111701, arXiv:1702.02699[hep-ph]; P. Ko, T. Nomura, and H. Okada, Phys. Lett. B, 772:547(2017), doi:10.1016/j.physletb.2017.07.021, arXiv:1701.05788[hep-ph]; Y. Tang and Y. L. Wu, Chin. Phys. C, 42(3):033104(2018) doi:10.1088/1674-1137/42/3/033104, arXiv:1705.05643[hep-ph]; C. W. Chiang, X. G. He, J. Tandean, and X. B. Yuan, Phys. Rev. D, 96(11):115022(2017), doi:10.1103/PhysRevD.96.115022, arXiv:1706.02696[hep-ph]; C. H. Chen and T. Nomura, Phys. Lett. B, 777:420(2018), doi:10.1016/j.physletb.2017.12.062, arXiv:1707.03249[hep-ph]; S. Baek, arXiv:1707.04573[hep-ph]; L. Bian, S. M. Choi, Y. J. Kang, and H. M. Lee, Phys. Rev. D, 96(7):075038(2017), doi:10.1103/PhysRevD.96.075038, arXiv:1707.04811[hep-ph]; G. Faisel and J. Tandean, JHEP, 1802:074(2018), doi:10.1007/JHEP02(2018)074, arXiv:1710.11102[hep-ph]; K. Fuyuto, H. L. Li, and J. H. Yu, arXiv:1712.06736[hep-ph]
[3]	S. Schael et al (ALEPH and DELPHI and L3 and OPAL and LEP Electroweak Collaborations), Phys. Rept., 532:119(2013), doi:10.1016/j.physrep.2013.07.004, arXiv:1302.3415[hep-ex]
[4]	M. Aaboud et al (ATLAS Collaboration), JHEP, 1710:182(2017), doi:10.1007/JHEP10(2017)182, arXiv:1707.02424[hep-ex]
[5]	L. Bian, H. M. Lee, and C. B. Park, arXiv:1711.08930[hep-ph]
[6]	C. Patrignani et al (Particle Data Group), Chin. Phys. C, 40(10):100001(2016)
[7]	F. Gabbiani, E. Gabrielli, A. Masiero, and L. Silvestrini, Nucl. Phys. B, 477:321(1996), doi:10.1016/0550-3213(96)00390-2,[hep-ph/9604387]
[8]	H. Baer et al, arXiv:1306.6352[hep-ph]
[9]	A. M. Baldini et al (MEG Collaboration), Eur. Phys. J. C, 76(8):434(2016) arXiv:1605.05081[hep-ex]
[10]	J. Adam et al (MEG Collaboration), Phys. Rev. Lett., 110:201801(2013), arXiv:1303.0754[hep-ex]
[11]	CMS Collaboration, Physics Analysis Summary CMS PAS EXO-12-061; G. Aad et al (ATLAS Collaboration), ATLAS-CONF-2013-017
[12]	W. Altmannshofer, S. Gori, M. Pospelov, and I. Yavin, Phys. Rev. Lett., 113:091801(2014), doi:10.1103/PhysRevLett.113.091801, arXiv:1406.2332[hep-ph]
[13]	C. W. Chiang and H. Okada, arXiv:1711.07365[hep-ph]
[14]	K. Hagiwara, R. Liao, A. D. Martin, D. Nomura, and T. Teubner, J. Phys. G, 38:085003(2011), doi:10.1088/0954-3899/38/8/085003, arXiv:1105.3149[hep-ph]
[15]	P. Arnan, L. Hofer, F. Mescia, and A. Crivellin, JHEP, 1704:043(2017), doi:10.1007/JHEP04(2017)043, arXiv:1608.07832[hep-ph]
[16]	S. Descotes-Genon, L. Hofer, J. Matias, and J. Virto, JHEP, 1606:092(2016), doi:10.1007/JHEP06(2016)092, arXiv:1510.04239[hep-ph]
[17]	D. S. Akerib et al (LUX Collaboration), Phys. Rev. Lett., 118(2):021303(2017), doi:10.1103/PhysRevLett.118.021303, arXiv:1608.07648[astro-ph.CO]
[18]	F. Giacchino, L. Lopez-Honorez, and M. H. G. Tytgat, JCAP, 1310:025(2013), doi:10.1088/1475-7516/2013/10/025, arXiv:1307.6480[hep-ph]
[19]	P. A. R. Ade et al (Planck Collaboration), Astron. Astrophys., 571:A16(2014), doi:10.1051/0004-6361/201321591, arXiv:1303.5076[astro-ph.CO]
[20]	CEPC-SPPC Study Group, IHEP-CEPC-DR-2015-01, IHEP-TH-2015-01, IHEP-EP-2015-01

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[17]	Deng Weizhen , Yang Zeshen , Wang Yucheng . A Non-Hermitian Approach of Dyson Boson Expansion in Interacting Boson Model. Chinese Physics C, 1993, 17(S3): 285-290.
[18]	Zheng Bo , Guo Shuohong . A Solvable 1 + 1 Dimensional U(l) gauge model. Chinese Physics C, 1990, 14(S1): 65-69.
[19]	Jing Sicong , and Ruan Tunan . Quantization of Pure Gauge Fields on Coset Space of Abelian Chiral Group. Chinese Physics C, 1988, 12(S4): 347-358.
[20]	Jin Changhao . Down-Quark Masses and Flavor Mixing. Chinese Physics C, 1988, 12(S1): 59-68.

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Linping Mu, Hiroshi Okada and Chao-Qiang Geng. A model with flavor-dependent gauged U(1)_B-L₁×U(1)_B-L₂-L₃ symmetry[J]. Chinese Physics C, 2018, 42(12): 123106. doi: 10.1088/1674-1137/42/12/123106

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Received: 2018-06-18
Revised: 2018-09-02

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Supported by National Center for Theoretical Sciences and MoST (MoST-104-2112-M-007-003-MY3 and MoST-107-2119-M-007-013-MY3)

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A model with flavor-dependent gauged U(1)_B-L₁×U(1)_B-L₂-L₃ symmetry

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A model with flavor-dependent gauged U(1)_B-L₁×U(1)_B-L₂-L₃ symmetry

Corresponding author: Linping Mu,

Corresponding author: Hiroshi Okada,

Corresponding author: Chao-Qiang Geng,

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