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Related papers: Tiny neutrino mass from SUSY and lepton number bre…

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Supersymmetric standard model with softly broken lepton symmetry provides a suitable framework to accommodate the solar and atmospheric neutrino anomalies. This model contains a natural explanation for large mixing and hierarchal masses…

High Energy Physics - Phenomenology · Physics 2009-10-31 Anjan S. Joshipura , Sudhir K. Vempati

We study a variation to the SUSY Left-Right symmetric model based on the gauge group $SU(3)_c\times SU(2)_L\times SU(2)_R\times U(1)_{BL}$. Beyond the quark and lepton superfields we only introduce a second Higgs bidoublet to produce…

High Energy Physics - Phenomenology · Physics 2016-03-09 Nobuchika Okada , Nathan Papapietro

We demonstrate that an $SU(2)_L\times U(1)_Y$ model with the same particle content as Standard Model(SM) and discrete reflection symmetry between second and third generation of leptons give rise to charged lepton and neutrino mass matrices…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ambar Ghosal

Radiative neutrino mass generation within supersymmetric (SUSY) construction is studied. The mechanism is considered where the lepton number violation is originating from the soft SUSY breaking terms. This requires MSSM extensions with…

High Energy Physics - Phenomenology · Physics 2017-01-04 Luka Megrelidze , Zurab Tavartkiladze

A generic form of the supersymmetric SM naturally gives rise to the lepton number violating neutrino masses and mixings, without the need for extra superfields beyond the minimal spectrum. Hence, SUSY can be consider the origin of beyond SM…

High Energy Physics - Phenomenology · Physics 2017-08-23 Otto C. W. Kong

In the Supersymmetric extension of the Standard Model with minimal particle content the three neutrinos can have non trivial masses and mixings, generated at 1 loop due to renormalizable lepton number violating interactions. We show that…

High Energy Physics - Phenomenology · Physics 2009-09-25 D. Tommasini

Lepton flavour violation and neutrino masses are a signal for new Physics beyond the Standard Model and are deeply related. The minimal extension of the Standard Model to make it include neutrino masses is not satisfactory from a conceptual…

High Energy Physics - Phenomenology · Physics 2011-07-29 J. N. Esteves

The addition of gauge singlet fermions to the Standard Model Lagrangian renders the neutrinos massive and allows one to explain all that is experimentally known about neutrino masses and lepton mixing by varying the values of the Majorana…

High Energy Physics - Phenomenology · Physics 2009-10-29 Andre de Gouvea , Wei-Chih Huang , James Jenkins

The notion of U(1) lepton number (which may only be softly broken) is applied to models of dark matter which interacts with leptons. Previous scotogenic models of Majorana or Dirac neutrino mass are shown to be derivable in this framework…

High Energy Physics - Phenomenology · Physics 2020-09-02 Ernest Ma

A spontaneously broken non-Abelian SU(3) family symmetry can generate a realistic form for quark, charged lepton and neutrino masses and mixing angles. It also gives a new solution to the SUSY flavour problem by ensuring near family…

High Energy Physics - Phenomenology · Physics 2009-11-10 M. R. Ramage , G. G. Ross

Heavy neutrinos from the Type-I Seesaw model can have a large mixing with active states, motivating their search at collider experiments. However, loop corrections to light neutrino masses constrain the heavy neutrinos to appear in…

High Energy Physics - Phenomenology · Physics 2023-06-14 J. Jones-Pérez , O. Suarez-Navarro

We investigate a simple model of neutrino mass based on SU(3)_C X SU(3)_L X U(1)_X gauge unification. The Yukawa coupling of the model has automatic lepton-number symmetry which is broken only by the self-couplings of the Higgs boson. At…

High Energy Physics - Phenomenology · Physics 2008-11-26 Darwin Chang , Hoang Ngoc Long

Recent data in the neutrino sector point towards a relatively large value of the reactor angle, incompatible with a vanishing theta_ 13 at about 3 sigma. In order to explain such a result, we propose a SUSY model based on the broken…

High Energy Physics - Phenomenology · Physics 2015-05-30 Davide Meloni

A new model for tiny neutrino masses is proposed in the gauge theory of $SU(3)_C \otimes SU(3)_L \otimes U(1)_X$, where neutrino masses are generated via the quantum effect of new particles. In this model, the fermion content is taken to be…

High Energy Physics - Phenomenology · Physics 2020-05-15 Arindam Das , Kazuki Enomoto , Shinya Kanemura , Kei Yagyu

Fermion masses and mixing angles including that of neutrinos are studied in a model with symmetry group SUSY $SO(10)\times \Delta (48) \times U(1)$. Universality of Yukawa coupling of superfields is assumed. The resulting texture of mass…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. C. Chou , Y. L. Wu

If there exist only three light neutrinos below the weak scale, the neutrino masses can arise by breaking the lepton number L. One example is the Zee mechanism for the neutrino masses. We study phenomenological implications of neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jihn E. Kim , Jae Sik Lee

Based on the stochastic superspace mechanism for softly breaking supersymmetry, we present improved sparticle spectra computations for the minimal model and examine extensions through R-parity violation and the type-I seesaw mechanism that…

High Energy Physics - Phenomenology · Physics 2015-03-13 Archil Kobakhidze , Nadine Pesor , Raymond R. Volkas

The radiatively induced neutrino mass matrix is investigated on the basis of an SU(5) SUSY model. In order to evade the proton decay, an ansatz based on a discrete symmetry $Z_2$ is assumed: although, at the unification scale, we have two…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide , Joe Sato

We study a neutrino mass model based on $S_4$ flavor symmetry which accommodates lepton mass, mixing with non-zero $\theta_{13}$ and CP violation phase. The spontaneous symmetry breaking in the model is imposed to obtain the realistic…

High Energy Physics - Phenomenology · Physics 2016-04-20 V. V. Vien

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
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