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Related papers: A See-saw model of sterile neutrino

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Some of basic problems in neutrino physics such as new energy scales, the enormous gap between neutrino masses and the lightest charged fermion mass, possible existance of sterile neutrinos in eV mass range are studied in the local gauge…

High Energy Physics - Phenomenology · Physics 2008-11-26 Riazuddin , Fayyazuddin

We studied a left-right symmetric model that can accommodate the neutrino dark energy (\nd) proposal. Type III seesaw mechanism is implemented to give masses to the neutrinos. After explaining the model, we study the consistency of the…

High Energy Physics - Phenomenology · Physics 2010-04-21 Jitesh R. Bhatt , Pei-Hong Gu , Utpal Sarkar , Santosh K. Singh

A simple renormalizable U(1) gauge model is constructed to explain the smallness of the active neutrino masses and provide the stable cold dark matter candidate simultaneously. The local U(1) symmetry is assumed to be spontaneously broken…

High Energy Physics - Phenomenology · Physics 2012-01-27 We-Fu Chang , Chi-Fong Wong

The usual see-saw mechanism for the generation of light neutrino masses is based on the assumption that all of the flavours of right-handed (more properly, sterile) neutrinos are heavy. If the sterile Majorana mass matrix is singular, one…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. H. J. McKellar , G. J. Stephenson , T. Goldman , M. Garbutt

Motivated by the short-baseline neutrino oscillation anomalies that suggest the existence of sterile neutrinos at the eV scale, we construct a scenario of a seesaw mechanism for 3+1 light neutrinos implemented by warped compactification of…

High Energy Physics - Phenomenology · Physics 2020-01-06 Shinsuke Kawai , Nobuchika Okada

We present a TeV-scale left-right ultraviolet completion of type-I seesaw for neutrino masses based on the $SU(2)_L\times SU(2)_R\times U(1)_{B-L}$ gauge group without parity, which leads to "large" light-heavy neutrino mixing while keeping…

High Energy Physics - Phenomenology · Physics 2013-12-04 P. S. Bhupal Dev , Chang-Hun Lee , R. N. Mohapatra

We consider an SU(3)'_c\times SU(2)'_L\times U(1)'_Y mirror sector where the field content and dimensionless couplings are a copy of the SU(3)_c\times SU(2)_L\times U(1)_Y ordinary sector. Our model also contains three gauge-singlet…

High Energy Physics - Phenomenology · Physics 2015-06-15 Pei-Hong Gu

In this letter, we introduce the ``flipped see-saw mechanism'', a new type of see-saw mechanism with 4th-generation neutrinos. This mechanism naturally explains the light sterile neutrino which is needed to account for all neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Stephen Godfrey , Shouhua Zhu

The possibility of generating neutrino mass through see-saw mechanism involving U(1) chiral Peccei-Quinn and scale symmetries breakdown is discussed. We consider a generic scale invariant model which has three Majorana fermions and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alex Gomes Dias

In this talk we assume the conventional see-saw mechanism, and contruct a hierarchical pattern of three active neutrinos with bi-maximal mixing. In order to enforce the hierarchy we use the single right handed neutrino dominance mechanism…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. F. King

Cosmological constraints on the sum of the neutrino masses can be relaxed if the number density of active neutrinos is reduced compared to the standard scenario, while at the same time keeping the effective number of neutrino species…

High Energy Physics - Phenomenology · Physics 2024-06-24 Miguel Escudero , Thomas Schwetz , Jorge Terol-Calvo

The singular see-saw mechanism is a variation of the see-saw mechanism whereby the right-chiral neutrino Majorana mass matrix is singular. Previous works employing the singular see-saw mechanism have assumed a vanishing left-chiral Majorana…

High Energy Physics - Phenomenology · Physics 2010-10-28 Kristian. L. McDonald , B. H. J. McKellar

In pursuit of a balance between theoretical naturalness and experimental testability, we propose two classes of multiple seesaw mechanisms at the TeV scale to understand the origin of tiny neutrino masses. They are novel extensions of the…

High Energy Physics - Phenomenology · Physics 2009-09-28 Zhi-zhong Xing , Shun Zhou

We present a grand unified model based on the supersymmetric $SU(3)_L\otimes SU(3)_{CL}\otimes SU(3)_{CR}\otimes SU(3)_R$ gauge group, which unifies in one single step the three gauge couplings of the standard model at an scale $M\sim…

High Energy Physics - Phenomenology · Physics 2009-10-31 Abdel Pérez-Lorenzana , William A. Ponce

Alternatives to the see-saw mechanism are explored in supersymmetric models with three right-handed or sterile neutrinos. Tree-level Yukawa couplings can be drastically suppressed in a natural way to give sub-eV Dirac neutrino masses. If,…

High Energy Physics - Phenomenology · Physics 2009-09-29 Francesca Borzumati , Yasunori Nomura

We propose a gauged $U(1)_{B-L}$ extension of the standard model (SM) to explain simultaneously the light neutrino masses and dark matter (DM). The generation of neutrino masses occurs through a variant of type-II seesaw mechanism in which…

High Energy Physics - Phenomenology · Physics 2020-02-18 Satyabrata Mahapatra , Nimmala Narendra , Narendra Sahu

We discuss phenomenology of the radiative seesaw model in which spontaneous breaking of the U(1)$_{B-L}$ gauge symmetry at the TeV scale gives the common origin for masses of neutrinos and dark matter (Kanemura et al., 2012). In this model,…

High Energy Physics - Phenomenology · Physics 2013-05-30 Shinya Kanemura , Takehiro Nabeshima , Hiroaki Sugiyama

We consider various possibilities for generating neutrino masses in supersymmetric models with an additional U(1)' gauge symmetry. One class of models involves two extra U(1)' x U(1)'' gauge symmetries, with U(1)'' breaking at an…

High Energy Physics - Phenomenology · Physics 2009-11-10 Junhai Kang , Paul Langacker , Tianjun Li

We propose a new scenario in a class of superstring derived standard--like models that explains the suppression of the left--handed neutrino masses. Due to nonrenormalizable terms and the breaking of the $U(1)_{Z^\prime}$ symmetry a…

High Energy Physics - Theory · Physics 2011-02-09 Alon E. Faraggi , Edi Halyo

The common lore in the literature of neutrino mass generation is that the canonical see-saw mechanism beautifully offers an explanation for the tiny neutrino mass but at the cost of introducing right-handed neutrinos at a scale that is out…

High Energy Physics - Phenomenology · Physics 2015-05-28 A. G. Dias , C. A. de S. Pires , P. S. Rodrigues da Silva
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