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

Abstract
HTML
Reference
Related

PDF

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

[1]	Takuya Morozumi , Hideaki Okane , Hiroki Sakamoto , Yusuke Shimizu , Kenta Takagi , Hiroyuki Umeeda . Phenomenological aspects of possible vacua of a neutrino flavor model. Chinese Physics C, 2018, 42(2): 023102. doi: 10.1088/1674-1137/42/2/023102
[2]	Jinn-Ouk Gong , Seong Chan Park . A minimal gauge inflation model. Chinese Physics C, 2018, 42(9): 095102. doi: 10.1088/1674-1137/42/9/095102
[3]	J. H. Field . A comparison of direct and indirect determinations of the masses of the Higgs Boson and the top quark. Chinese Physics C, 2017, 41(10): 103001. doi: 10.1088/1674-1137/41/10/103001
[4]	DING Gui-Jun , ZHOU Ye-Ling . Predicting lepton flavor mixing from Δ(48) and generalized CP symmetries. Chinese Physics C, 2015, 39(2): 021001. doi: 10.1088/1674-1137/39/2/021001
[5]	WANG Hai-Peng , YUN Ming-Kai , LIU Shuang-Quan , FAN Xin , CAO Xue-Xiang , CHAI Pei , SHAN Bao-Ci . A region segmentation based algorithm for building a crystal position lookup table in a scintillation detector. Chinese Physics C, 2015, 39(3): 038201. doi: 10.1088/1674-1137/39/3/038201
[6]	HOU Jia-Xun , PENG Guang-Xiong , XIA Cheng-Jun , XU Jian-Feng . Magnetized strange quark matter in a mass-density-dependent model. Chinese Physics C, 2015, 39(1): 015101. doi: 10.1088/1674-1137/39/1/015101
[7]	DENG Jun , CAO Lei , SU Xu . Monte Carlo simulation of indoor external exposure due to gamma-emitting radionuclides in building materials. Chinese Physics C, 2014, 38(10): 108202. doi: 10.1088/1674-1137/38/10/108202
[8]	CHEN Yan-Jun . Quasielastic electron scattering in a derivative coupling model with relativistic random phase approximation. Chinese Physics C, 2013, 37(7): 074101. doi: 10.1088/1674-1137/37/7/074101
[9]	CHAO Wei . Neutrino masses and lepton-flavor-violating τ decays in the supersymmetric left-right model. Chinese Physics C, 2011, 35(3): 214-222. doi: 10.1088/1674-1137/35/3/002
[10]	WANG Shuai-Wei , YANG Xing-Qiang , LI Gen-Quan , HUANG Jin-Shu . B_s,d→μ⁺μ^－ decays in a flavor changing Z′ model. Chinese Physics C, 2010, 34(5): 539-542. doi: 10.1088/1674-1137/34/5/004
[11]	ZHANG Zhen-Xia , BIAN Jian-Guo , CHEN Guo-Ming , CHEN Ming-Shui , LI Zu-Hao , LIANG Song , MENG Xiang-Wei , QI Yong-Hui , TANG Zhi-Cheng , TAO Jun-Quan , WANG Jian , WANG Zheng , WANG Xian-You , WANG Jian-Xiong , XIAO Hong , YANG Min , ZANG Jing-Jing , ZHANG Bin , ZHANG Zhen . Study of new boson W^±₁ in the Minimal Higgsless Model at the LHC. Chinese Physics C, 2010, 34(4): 427-432. doi: 10.1088/1674-1137/34/4/002
[12]	WANG Qing , WANG Shun-Zhi , ZHANG Ying . New gauge forces beyond the standard model. Chinese Physics C, 2010, 34(2): 277-286. doi: 10.1088/1674-1137/34/2/025
[13]	LIU Wei , YUE Chong-Xing , SU Xue-Song , WANG Yong-Zhi . LHT model and Higgs boson production in association with a weak gauge boson at the LHC. Chinese Physics C, 2010, 34(10): 1565-1569. doi: 10.1088/1674-1137/34/10/003
[14]	WANG Ke , JIANG Yun-Guo , HUO Qiu-Hong . Quantal symmetries in the non-linear σ model with Maxwell and non-Abelian Chern-Simons terms. Chinese Physics C, 2010, 34(5): 535-538. doi: 10.1088/1674-1137/34/5/003
[15]	WANG Xue-Lei , JIN Zhen-Lan , ZENG Qing-Guo . Production of the new gauge boson B_H via e^－ collision in the littlest Higgs model. Chinese Physics C, 2008, 32(3): 165-171. doi: 10.1088/1674-1137/32/3/001
[16]	Chen Xingqu , Xing Zheng . Analysis of Superdeformed Bands in the Particle-Rotor Model. Chinese Physics C, 1994, 18(Z1): 95-102.
[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]	Fan Qinmin , Zhong Ming . The Use of Numerical Calculation in the Analysis of Standardless Thick Target PIXE. Chinese Physics C, 1988, 12(S2): 109-116.
[20]	Jin Changhao . Down-Quark Masses and Flavor Mixing. Chinese Physics C, 1988, 12(S1): 59-68.

Access

Get Citation

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

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

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

Fund

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

Article Metric

Article Views(1613)
PDF Downloads(14)
Cited by(0)

Policy on re-use

To reuse of Open Access content published by CPC, for content published under the terms of the Creative Commons Attribution 3.0 license (“CC CY”), the users don’t need to request permission to copy, distribute and display the final published version of the article and to create derivative works, subject to appropriate attribution.

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

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

Abstract：

References

Access

Article Metrics

Metrics

通讯作者: 陈斌, bchen63@163.com

Email This Article

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,

HTML

目录