English
Related papers

Related papers: Neutrino Masses and Helicities

200 papers

One can describe cosmological relic neutrinos by adding Lagrange multipliers to the Standard Model Lagrangian for them. The two possible Lagrange multipliers are a chemical potential, which fixes the mean neutrino/anti-neutrino asymmetry,…

High Energy Physics - Phenomenology · Physics 2013-02-13 Bob McElrath

We extend the Private Higgs scenario to account for charged lepton and neutrino masses by introducing a private Higgs field for each lepton family. We analyze a model in which neutrino Majorana masses are radiatively induced. Contrary to…

High Energy Physics - Phenomenology · Physics 2009-01-21 Rafael A. Porto , A. Zee

If neutrinos are Dirac fermions, certain new physics beyond the standard model should exist to account for the smallness of neutrino mass. With two additional scalars and a heavy intermediate fermion, in this paper, we systematically study…

High Energy Physics - Phenomenology · Physics 2017-05-02 Weijian Wang , Zhi-Long Han

The electroweak unification group $G\equiv SU(2)_L\times U(1)_e\times U(1)_\mu\times U(1)_\tau$ in which each fermion multiplet has its own $U(1)$ factor was proposed in 1986 to get the neutrino mass matrix. In this paper, the gauge group G…

High Energy Physics - Phenomenology · Physics 2019-06-26 Fayyazuddin

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

The mass-varying neutrino scenario is analyzed for three trial quintessence potentials (Ferreira-Joyce, inverse exponential, and thawing oscillating). The neutrino mass is generated via Yukawa coupling to the scalar field which represents…

High Energy Physics - Phenomenology · Physics 2021-05-19 Sayan Mandal , Gennady Y. Chitov , Olga Avsajanishvili , Bijit Singha , Tina Kahniashvili

If three right-handed neutrinos are added to the Standard Model, then, for the three known generations, there are six quarks and six leptons. It is then natural to assume that the symmetry considerations that have been applied to the quark…

High Energy Physics - Phenomenology · Physics 2007-05-23 Per Osland , Tai Tsun Wu

The possible mechanisms of generation of the neutrino of small masses and sterile neutrino are considered. In the supposition of stability of tracks of a left-right symmetry concerning masses of constituent quarks, the angles of mixing of…

High Energy Physics - Phenomenology · Physics 2015-05-13 Vladimir Efrosinin

In this talk we explore the possibility that the smallness of the observed neutrino masses is naturally understood in a modified version of the standard model with N extra generations of fermions and N right-handed neutrinos, in which light…

High Energy Physics - Phenomenology · Physics 2014-10-15 A. Aparici , J. Herrero-Garcia , N. Rius , A. Santamaria

In practically all extentions of the standard model, the neutrinos naturally acquire a mass. The neutrino mass matrix, however, contains many parameters which can neither be predicted by the prevailing models nor can be fitted to the data.…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. K. Leontaris , J. D. Vergados

The origin of the neutrino mass, dark matter (DM), and dark energy (DE) are among the most challenging problems of fundamental physics. We address these questions from analyses of the models where the neutrino mass is generated via Yukawa…

High Energy Physics - Phenomenology · Physics 2012-01-23 Gennady Y. Chitov

We explore generating the dimension five operator leading to neutrino masses by integrating out heavy SU(2)_L triplet fermions. We exhibit a model that has a neutrino mass matrix consistent with observations. In addition, the model is…

High Energy Physics - Phenomenology · Physics 2008-12-30 Willy Fischler , Raphael Flauger

In the recent note we argued that most of the available positive and negative neutrino oscillation data can be incorporated in a four-neutrino weak interaction model with one physical condition: thorough maximal mixing of the neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. M. Lipmanov

Quantum field theory of space-like particles is investigated in the framework of absolute causality scheme preserving Lorentz symmetry. It is shown that tachyons are associated with unitary orbits of Poincar\'e mappings induced from SO(2)…

High Energy Physics - Phenomenology · Physics 2008-02-03 J. Rembielinski

A new mechanism is proposed for generating neutrino masses radiatively through a non-minimal coupling to gravity of fermionic bilinears involving massive neutral fermions. Such coupling terms can arise in theories where the gravity sector…

High Energy Physics - Phenomenology · Physics 2008-11-26 Abhinav Gupta , Namit Mahajan , Amitabha Mukherjee

We present a comprehensive study of five-dimensional brane-world models for neutrino physics based on flat compactifications. Particular emphasis is put on the inclusion of bulk mass terms. We derive a number of general results for such…

High Energy Physics - Phenomenology · Physics 2010-02-03 Andre Lukas , Pierre Ramond , Andrea Romanino , Graham G. Ross

Motivated by the Super-Kamiokande data, we revisit models with U(1) symmetries and discuss the origin of neutrino masses and mixings in such theories. We show that, in models with just three light neutrinos and a hierarchy of neutrino…

High Energy Physics - Phenomenology · Physics 2009-10-31 Smaragda Lola , Graham G. Ross

In this paper, we move from a "proof of concept" to challenging predictions in a flavour model emerging from a single fermion family in six dimensions (6-D) with the two extra dimensions compactified on a sphere. The most striking…

High Energy Physics - Phenomenology · Physics 2013-08-21 J. -M. Frere , M. Libanov , S. Mollet , S. Troitsky

A mechanism of radiatively generating neutrino masses is implemented in an SU(2)_L x U(1)_Y x SU(2)'_L x U(1)'_Y model, where the first and second families respect SU(2)_L x U(1)_Y while SU(2)'_L x U(1)'_Y is specific for the third family.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yutaka Okamoto , Masaki Yasue

We discuss what kinds of combinations of Yukawa interactions can generate the Majorana neutrino mass matrix. We concentrate on the flavor structure of the neutrino mass matrix because it does not depend on details of the models except for…

High Energy Physics - Phenomenology · Physics 2016-01-20 Shinya Kanemura , Hiroaki Sugiyama
‹ Prev 1 3 4 5 6 7 10 Next ›