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Related papers: Could a Slepton be the Zee boson?

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A heavy triplet of leptons $(\Sigma^+, \Sigma^0, \Sigma^-)_R$ per family is proposed as the possible anchor of a small seesaw neutrino mass. A new U(1) gauge symmetry is then also possible, and the associated gauge boson $X$ may be…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma , D. P. Roy

Some supersymmetric models after the recent LHC reports are discussed. Especially, the light Higgs boson around 125GeV is attempted to be accommodated. An extra Z' from GUTs, and the scalar and pseudoscalar Higgs bosons in supersymmetric…

High Energy Physics - Phenomenology · Physics 2015-06-05 Jihn E. Kim

If supersymmetry (SUSY) is not for stabilizing the electroweak energy scale, what is it used for in particle physics? We propose that it is for flavor problems. A cyclic family symmetry is introduced. Under the family symmetry, only the…

High Energy Physics - Phenomenology · Physics 2009-11-11 Chun Liu

Charged scalar particles introduced in some extensions of the standard model can induce $\tau$ leptonic decay at tree level. We find that with some charged SU(2)-singlet scalar particles, like ones introduced in Zee-type models, $\tau$…

High Energy Physics - Phenomenology · Physics 2009-10-22 Zhijian Tao

The recent discovery by SuperKamiokande of evidence for neutrino masses requires the addition of at least seven new parameters to the Standard Model. We discuss the general theoretical schemes which require their inclusion, and point out…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Ramond

We discuss type-II seesaw models adopting modular $A_4$ symmetry in supersymmetric framework. In our approach, the models are classified by the assignment of $A_4$ representations and modular weights for leptons and triplet Higgs fields.…

High Energy Physics - Phenomenology · Physics 2020-08-26 Tatsuo Kobayashi , Takaaki Nomura , Takashi Shimomura

The $U(1)_{B\textrm{--}L}$ symmetry, the essential component in the seesaw mechanism and leptogenesis, is naturally equipped with a massive gauge boson. If this gauge boson is the dark matter, the scenario consistent with the seesaw…

High Energy Physics - Phenomenology · Physics 2022-10-14 Weikang Lin , Luca Visinelli , Donglian Xu , Tsutomu T. Yanagida

We build a supersymmetric version with $SU(3)_C\otimes SU(2)_L\otimes U(1)_{Y^\prime}\otimes U(1)_{B-L}$ gauge symmetry, where $Y^\prime$ is a new charge and $B$ and $L$ are the usual baryonic and leptonic numbers. The model has three…

High Energy Physics - Phenomenology · Physics 2017-06-14 J. C. Montero , V. Pleitez , M. C. Rodriguez , B. L. Sánchez-Vega

We study the scalar potential and the mass spectrum of the supersymmetric extension of a three-family model based on the local gauge group $SU(3)_C\otimes SU(3)_L\otimes U(1)_X$, with anomalies canceled among the three families in a…

High Energy Physics - Phenomenology · Physics 2011-09-13 Luis A. Sanchez , William A. Ponce , Jesus M. Mira

The origin of neutrino masses is currently one of the most intriguing questions of particle physics and many extensions of the Standard Model have been proposed in that direction. This experimental evidence is a very robust indication of…

High Energy Physics - Phenomenology · Physics 2015-03-19 Avelino Vicente

To generate small neutrino masses radiatively, the Zee-model introduces two Higgs doublets and one weak-singlet charged Higgs boson to its Higgs sector. From analyzing the renormalization group equations, we determine the possibile range of…

High Energy Physics - Phenomenology · Physics 2009-10-31 Shinya Kanemura , Takashi Kasai , Guey-Lin Lin , Yasuhiro Okada , Jie-Jun Tseng , C. -P. Yuan

We follow a minimalistic approach to neutrino masses, by introducing a single heavy singlet $N$ into the standard model (or supersymmetric standard model) with a heavy Majorana mass $M$, which couples as a single right-handed neutrino in a…

High Energy Physics - Phenomenology · Physics 2009-10-31 S. F. King

In this talk I discuss the qualitative features of an SO(10) SUSY GUT with an SU(2)x U(1)$^n$ family symmetry. I then describe the global fit of this theory to precision electroweak data [including charged fermion masses and mixing angles].…

High Energy Physics - Phenomenology · Physics 2009-10-31 Stuart Raby

Any new neutrino physics at the TeV scale must include a suppression mechanism to keep its contribution to light neutrino masses small enough. We review some seesaw model examples with weakly broken lepton number, and comment on the…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. del Aguila , J. A. Aguilar Saavedra , J. de Blas , M. Zralek

We study a seesaw-type extension of the Standard Model in which the symmetry group is enlarged by a global U(1). We introduce adequate scalar and fermion representations which naturally explain the smallness of neutrino masses. With the…

High Energy Physics - Phenomenology · Physics 2011-12-19 François-Xavier Josse-Michaux , Emiliano Molinaro

We study the impact of Standard Model singlet neutrinos on neutrino flavor transformation. We focus on an extension of the Zee model which includes singlet neutrinos, and find that the best limits on the interactions of the singlet…

High Energy Physics - Phenomenology · Physics 2009-10-31 G. C. McLaughlin , J. N. Ng

I review promising approaches to neutrino mass models, focussing on three neutrino patterns of neutrino masses and mixing angles, and the corresponding Majorana mass matrices. I discuss the see-saw mechanism, and show how it may be applied…

High Energy Physics - Phenomenology · Physics 2015-06-25 S. F. King

Naturally small neutrino masses can arise in some grand unified models. The mechanism of neutrino mass generation in these models typically requires the existence of neutral heavy leptons. We study the low-energy phenomenology of these new…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ivan Melo

We suggest that a singlet fermion $S$ exists beyond the standard see-saw structure. It mixes with light neutrinos via interactions with the right-handed neutrino components, so that $\n_e \to S$ conversion solves the solar neutrino problem.…

High Energy Physics - Phenomenology · Physics 2009-10-28 E. J. Chun , Anjan S. Joshipura , A. Yu. Smirnov

Adding a second scalar doublet (eta^+,eta^0) and three neutral singlet fermions N_{1,2,3} to the Standard Model of particle interactions with a new Z_2 symmetry, it has been shown that Re(eta^0) or Im(eta^0) is a good dark-matter candidate…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernest Ma
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