Fermions, Gauge Bosons and Higgs Masses in the 3-3-1-1 Model with Charged Lepton
Main Article Content
Abstract
A new version of 3-3-1-1 model proposed can solve the Landau pole problem of the previous versions. The masses of fermions are calculated in detail where the masses of active neutrinos are generated through the seesaw mechanism. All the Higgs bosons and gauge bosons as well as their masses are identified and calculated.
Keywords:
3-3-1-1 model, new charged leptons
References
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[23] G. Aad et al. (ATLAS Collaboration), Observation of a New Particle in the Search for the Standard Model Higgs Boson with the ATLAS Detector at the LHC, Phys. Lett. B, Vol. 716,No. 1, 2012, pp. 1-29, https://doi.org/10.1016/ j.physletb.2012.08.020.
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[2] R. Foot, H. N. Long, T. A. Tran, and Gauge Models with Right-Handed Neutrinos, Phys. Rev. D, Vol. 50, No. 1, 1994, pp.34-38, https://doi.org/10.1103/PhysRevD.50.R34.
[3] F. Pisano, V. Pleitez, An Model for Electroweak Interactions,Phys. Rev. D, Vol. 46, No. 1, 1992, pp. 410-417, https://doi.org/10.1103/PhysRevD.46.410.
[4] P. H. Frampton, Chiral Dilepton Model and the Flavor Question, Phys. Rev. Lett, Vol. 69, No. 20, 1992, pp. 2889-2891, https://doi.org/10.1103/PhysRevLett.69.2889.
[5] R. Foot, O. F. Hernandez, F. Pisano, V. Pleitez, Lepton Masses in an Gauge Model, Phys. Rev. D, Vol. 47, No. 9, 1993, pp. 4158-4161, https://doi.org/10.1103/PhysRevD.47.4158.
[6] J. C. Montero, F. Pisano, V. Pleitez, Neutral Currents and Gim Mechanism in Models for Electroweak Interactions, Phys. Rev. D, Vol. 47, No. 7, 1993, pp. 2918-2929, https://doi.org/10.1103/PhysRevD.47.2918.
[7] H. N. Long, Model for Right-Handed Neutrino Neutral Currents,Phys. Rev. D, Vol. 54, No. 7, 1996, pp. 4691-4693, https://doi.org/10.1103/PhysRevD.54.4691.
[8] P. V. Dong, H. T. Hung, T. D. Tham, 3-3-1-1 Model for Dark Matter, Phys. Rev. D, Vol.87, No. 11, 2013, pp. 115003_1 - 115003_17, https://doi.org/10.1103/PhysRevD.87.115003.
[9] P. V. Dong, D. T. Huong, F. S. Queiroz, N. T. Thuy, Phenomenology of the 3-3-1-1 Model, Phys. Rev. D, Vol. 90,No. 7, 2014, pp. 075021_1 – 075021_35, https://doi.org/10.1103/PhysRevD.90.075021.
[10] D. T. Huong, P. V. Dong, C. S. Kim, N. T. Thuy, Inflation and Leptogenesis In The3-3-1-1 Model, Phys. Rev. D, Vol.91, No. 5, 2015, pp. 055023_1 – 055023_19, https://doi.org/10.1103/PhysRevD.91.055023.
[11] P. V. Dong, Unifying the Electroweak and B-L Interactions, Phys. Rev. D, Vol. 92, No. 5, 2015, pp. 055026_1 – 055026_15, https://doi.org/10.1103/PhysRevD.92.055026.
[12] P. V. Dong, D. T. Si, Discriminating the Minimal 3-3-1 Models, Phys. Rev. D, Vol. 90, No. 11, 2014, pp. 117703_1 – 117703_4, https://doi.org/10.1103/PhysRevD.90.117703.
[13] P. V. Dong, D. T. Si, Kinetic Mixing Effect in the 3-3-1-1 Model, Phys. Rev. D, Vol. 93, No. 11, 2016, pp. 115003_1 – 115003_11, https://doi.org/10.1103/PhysRevD.93.115003.
[14] P. V. Dong, H. N. Long, Invariance and Models with Beta Arbitrary, Eur. Phys. J. C, Vol.42, No. 8, 2005, pp. 325-329, https://doi.org/10.1140/epjc/s2005-02314-x.
[15] K. Sasaki, Effects of Dilepton Gauge Bosons on the Electroweak Parameters S, T and U, Phys. Lett. B, Vol. 308, No. 3,1993, pp. 297-303, https://doi.org/10.1016/0370-2693(93)91288-X.
[16] P. H. Frampton, M. Harada, Constraints from Precision Electroweak Data on Leptoquarks and Bileptons, Phys. Rev. D, Vol. 58, No. 9, 1998,pp. 095013_1 – 095013_27, https://doi.org/10.1103/PhysRevD.58.095013.
[17] H.N. Long, T. Inami, S, T, U Parameters in Model with Right-Handed Neutrinos, Phys. Rev. D, Vol. 61, No. 7, 2000, p. 075002 (9 pages), https://doi.org/10.1103/PhysRevD.61.075002.
[18] M. Tanabashi et al. [Particle Data Group], Review of Particle Physics, Phys. Rev. D, Vol. 98, No. 3,pp. 030001_1 – 030001_1898 pages, 2018, https://doi.org/10.1103/PhysRevD.98.030001.
[19] M. Gell-Mann, P. Ramond, R. Slansky, Complex Spinors and Unified Theories, In Supergravity, edited by P. van Nieuwenhuizen and D. Z. Freedman, North Holland press, Amsterdam, 1979, pp. 315-321. [Published in: Conf.Proc.C 790927 (1979) 315-321].
[20] T. Yanagida, in Proceedings of the Workshop on the Unified Theory and the Baryon Number in the Universe, edited by O. Sawada and A. Sugamoto, KEK, Tsukuba, Japan, 1979, pp. 95-99.[Published in: Conf.Proc.C 7902131 (1979) 95-99].
[21] S. L. Glashow, The Future of Elementary Particle Physics, in Proceedings of the 1979 Cargèse Summer Institute on Quarks and Leptons, edited by M. Lévy, Plenum Press, New York, 1980, pp. 687-713.[Published in: NATO Sci. Ser. B 61 (1980) 687]
[22] R. N. Mohapatra, G. Senjanovié, Neutrino Mass and Spontaneous Parity Violation, Phys. Rev. Lett, Vol. 44, No. 14, 1980, pp. 912_1 – 912_10, https://doi.org/10.1103/PhysRevLett.44.912.
[23] G. Aad et al. (ATLAS Collaboration), Observation of a New Particle in the Search for the Standard Model Higgs Boson with the ATLAS Detector at the LHC, Phys. Lett. B, Vol. 716,No. 1, 2012, pp. 1-29, https://doi.org/10.1016/ j.physletb.2012.08.020.
[24] S. Chatrchyan et al. (CMS Collaboration), Observation of a New Boson at a Mass of 125 GeV with the CMS Experiment at the LHC, Phys. Lett. B, Vol. 716, No. 1, 2012, pp. 30-61, https://doi.org/10.1016/ j.physletb.2012.08.021.