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Related papers: Renormalization Group Evolution of the Non-Unitary…

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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,…

High Energy Physics - Phenomenology · Physics 2021-03-31 M. C. Rodriguez

The renormalization group evolution equation for two neutrino mixing is known to exhibit nontrivial fixed point structure corresponding to maximal mixing at the weak scale. The presence of the fixed point provides a natural explanation of…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. R. S. Balaji , R. N. Mohapatra , M. K. Parida , E. A. Paschos

A minimal version of the inverse seesaw model featuring only two pairs of TeV-scale singlet neutrinos is discussed from the perspective of non-standard neutrino interactions. A particular attention is paid to the non-standard patterns of…

High Energy Physics - Phenomenology · Physics 2014-11-20 Michal Malinsky

A nonuniversal abelian extension $\mathrm{U(1)}_{X}$ free from chiral anomalies is introduced into the Standard Model (SM), in order to evaluate its suitability in addressing the fermion mass hierarchy (FMH) by using seesaw mechanisms…

High Energy Physics - Phenomenology · Physics 2018-08-08 Carlos E. Díaz , S. F Mantilla , R. Martinez

There are no upper limits on the possible number of massive, singlet (right--handed) neutrinos that may participate in the seesaw mechanism, and some string constructions motivate seesaw models with up to O(100) right--handed neutrinos. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 John Ellis , Oleg Lebedev

If the only contribution to neutrinoless double beta decay (NLDBD) are neutrino masses its discovery may be very difficult, especially if neutrinos present a normal hierarchy spectrum. However, this is not the only possibility; NLDBD can in…

High Energy Physics - Phenomenology · Physics 2013-05-22 F. del Águila , A. Aparici , S. Bhattacharya , A. Santamaria , J. Wudka

The renormalization of general theories with inter-family mixing of Dirac and/or Majorana fermions is studied at the one-loop electroweak order. The phenomenological significance of the mixing-matrix renormalization is discussed, within the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Bernd A. Kniehl , Apostolos Pilaftsis

We derive the lepton number violating dimension-five and dimension-seven operators, relevant for neutrino mass generation, in the Minimal Supersymmetry Standard Model without R-parity (the $/R$MSSM) by using the effective Lagrangian method.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tai-Fu Feng , Jukka Maalampi

We propose a scalar Triplet extension of the standard model (SM) to unify the origin of neutrino mass with the visible and dark matter component of the Universe. We assume that the scalar triplet is super heavy, so that its CP-violating…

High Energy Physics - Phenomenology · Physics 2012-12-18 Narendra Sahu

The large mixing in the lepton sector observed in the recent neutrino-oscillation experiments strongly suggest that nature of left-handed lepton doublets is very different from that of left-handed quark doublets. This means that there is a…

High Energy Physics - Phenomenology · Physics 2010-11-19 T. Watari , T. Yanagida

The R-symmetry formalism is applied for the supersymmetric SU(3)_C X SU(3)_L X U(1)_X (3-3-1) model with right-handed neutrinos. For this kind of models, we study generalization of the MSSM relation among R-parity, spin and matter-parity.…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. V. Dong , D. T. Huong , M. C. Rodriguez , H. N. Long

Conventionally, neutrino masses in a supersymmetric theory arise from non-renormalizable lepton-number (L)-violating operators in the superpotential. The alternative possibility of having such operators in the Kahler potential as the…

High Energy Physics - Phenomenology · Physics 2009-11-07 J. A. Casas , J. R. Espinosa , I. Navarro

We discuss the simplest models for the generation of neutrinos masses at tree level and one-loop level. The realization of the different seesaw mechanisms in the context of renormalizable SU(5) and SO(10) theories is reviewed. A new…

High Energy Physics - Phenomenology · Physics 2010-05-07 Pavel Fileviez Perez

There are three observables related to neutrino mass, namely the kinematic mass in direct searches, the effective mass in neutrino-less double beta decay, and the sum of neutrino masses in cosmology. In the limit of exactly degenerate…

High Energy Physics - Phenomenology · Physics 2010-05-12 Werner Rodejohann

We study the renormalization of the $llHH$-type Majorana neutrino mass operator in a scenario where there is a compactified extra dimension and the fields involved correspond to only the standard model particles and their Kaluza-Klein…

High Energy Physics - Phenomenology · Physics 2009-11-07 Gautam Bhattacharyya , Srubabati Goswami , Amitava Raychaudhuri

We present the general form of the unitary matrices keeping invariant the Majorana neutrino mass matrix of specific texture suitable for explaining oscillation data. In the case of the Tri-bimaximal pattern with two degenerate masses we…

High Energy Physics - Phenomenology · Physics 2011-02-01 E. I. Lashin , S. Nasri , E. Malkawi , N. Chamoun

The Standard Model includes neutrinos as massless particles, but neutrino oscillations showed that neutrinos are not massless. A simple extension of adding gauge singlet fermions to the particle spectrum allows normal Yukawa mass terms for…

High Energy Physics - Phenomenology · Physics 2012-12-24 D. Jurciukonis , T. Gajdosik , A. Juodagalvis , T. Sabonis

We introduce a method to extract the right-handed neutrino mass matrix from the Left-Right symmetric seesaw formula and apply it to the study of a simple SUSY SO(10) theory. We find 8 possible solutions for the heavy neutrino spectrum and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pierre Hosteins

The current work involves augmenting the $\Delta(54)$ discrete flavor model by incorporating two Standard Model Higgs particles into the Inverse Seesaw mechanism. We introduced Weyl fermions and Vector like fermions, which are gauge…

High Energy Physics - Phenomenology · Physics 2024-03-01 Hrishi Bora , Ng. K. Francis , Bikash Thapa , Shawan Kumar Jha

The seesaw mechanism can play a key role in the generation of the leptonic mixing in unified models. We consider an unified model with a family symmetry and extended seesaw, and obtain viable fermion masses and mixing (leptonic mixing is…

High Energy Physics - Phenomenology · Physics 2015-05-14 Ivo de Medeiros Varzielas