We propose a classically conformal model in a minimal radiative seesaw, in which we employ a gauged B−L symmetry in the standard model that is essential in order to work the Coleman–Weinberg mechanism well that induces the B−L symmetry breaking. As a result, nonzero Majorana mass term and electroweak symmetry breaking simultaneously occur. In this framework, we show a benchmark point to satisfy several theoretical and experimental constraints. Here theoretical constraints represent inert conditions and Coleman–Weinberg condition. Experimental bounds come from lepton flavor violations (especially μ→eγ), the current bound on the Z′ mass at the CERN Large Hadron Collider, and neutrino oscillations
The Standard Model with an added Higgs portal interaction and no explicit mass terms is a classicall...
We revisit the relation between the neutrino masses and the spontaneous breaking of the B–L gauge sy...
We study a radiative seesaw model at one-loop level with a flavor dependent gauge symmetry U(1)μ−τ, ...
AbstractWe propose a classically conformal model in a minimal radiative seesaw, in which we employ a...
AbstractMany studies have been made on extensions of the standard model with B−L gauge symmetry. The...
Under the assumption of classical conformal invariance, we study the Coleman-Weinberg symmetry break...
We propose a model based on an alternative U(1)B−L gauge symmetry with 5 dimensional operators in th...
In order to address the hierarchy problem and to simultaneously explain small neutrino masses, we st...
Radiative neutrino mass models and the seesaw models are viewed from the unifying framework of stand...
The standard model Higgs mass term receives quadratically divergent radiative corrections, thereby d...
AbstractWe extend the Type I seesaw and suggest a new seesaw mechanism to generate neutrino masses w...
Abstract We study the minimal seesaw model, where two right-handed Majorana neutrinos are introduced...
We propose a radiative seesaw model in an alternative left–right model without any bidoublet scalar ...
The Standard Model (SM) of particle physics is a precise model of electroweak interactions. However,...
In the context of Standard Model (SM) extensions, the seesaw mechanism provides the most natural exp...
The Standard Model with an added Higgs portal interaction and no explicit mass terms is a classicall...
We revisit the relation between the neutrino masses and the spontaneous breaking of the B–L gauge sy...
We study a radiative seesaw model at one-loop level with a flavor dependent gauge symmetry U(1)μ−τ, ...
AbstractWe propose a classically conformal model in a minimal radiative seesaw, in which we employ a...
AbstractMany studies have been made on extensions of the standard model with B−L gauge symmetry. The...
Under the assumption of classical conformal invariance, we study the Coleman-Weinberg symmetry break...
We propose a model based on an alternative U(1)B−L gauge symmetry with 5 dimensional operators in th...
In order to address the hierarchy problem and to simultaneously explain small neutrino masses, we st...
Radiative neutrino mass models and the seesaw models are viewed from the unifying framework of stand...
The standard model Higgs mass term receives quadratically divergent radiative corrections, thereby d...
AbstractWe extend the Type I seesaw and suggest a new seesaw mechanism to generate neutrino masses w...
Abstract We study the minimal seesaw model, where two right-handed Majorana neutrinos are introduced...
We propose a radiative seesaw model in an alternative left–right model without any bidoublet scalar ...
The Standard Model (SM) of particle physics is a precise model of electroweak interactions. However,...
In the context of Standard Model (SM) extensions, the seesaw mechanism provides the most natural exp...
The Standard Model with an added Higgs portal interaction and no explicit mass terms is a classicall...
We revisit the relation between the neutrino masses and the spontaneous breaking of the B–L gauge sy...
We study a radiative seesaw model at one-loop level with a flavor dependent gauge symmetry U(1)μ−τ, ...