The scotogenic model of neutrino mass is modified so that the dark Majorana fermion singlet $S$ which makes the neutrino massive is itself generated in one loop. This is accomplished by having $Z_6$ lepton symmetry softly broken to $Z_2$ in the scalar sector by a unique quadratic term. It is shown that $S$ is a viable freeze-in dark-matter candidate through Higgs decay.Comment: 11 pages, 6 figure
The $SU(3)_c^{}\times SU(2)_L^{} \times U(1)_Y^{}$ standard model is extended by a $U(1)_{B-L}^{}$ g...
In this paper we propose a possible explanation of the active neutrino Majorana masses with the TeV ...
In this paper we propose a possible explanation of the active neutrino Majorana masses with the TeV ...
If dark matter is light, it may be due to a seesaw mechanism just as neutrinos are. It is postulated...
We study a one-loop induced neutrino mass model with an inert isospin triplet scalar field of $Y=0$ ...
Searches for Dark Matter suggest that it couples to ordinary matter only very weakly and possibly on...
We show that the minimal Type-I Seesaw mechanism can successfully account for the observed dark matt...
We extend the Dirac Scotogenic model with the aim of realizing neutrino masses together with the mas...
The hierarchy in scale between atmospheric and solar neutrino mass splittings is investigated throug...
We present a three-loop model of neutrino mass whose most-general Lagrangian possesses a softly-brok...
We propose an extension of the standard model (SM) by including a dark sector comprised of three gen...
AbstractA new and radical scenario of the simple 2006 model of radiative neutrino mass is proposed, ...
We explore a gauged $U(1)_{B-L}$ extension of standard model with inclusion of three right-handed ne...
The scotogenic model presents an elegant and succinct framework for elucidating the origin of tiny n...
We discuss the impact of neutrino phenomenology and related cosmology on a $A_{4}\otimes Z_{8}$ symm...
The $SU(3)_c^{}\times SU(2)_L^{} \times U(1)_Y^{}$ standard model is extended by a $U(1)_{B-L}^{}$ g...
In this paper we propose a possible explanation of the active neutrino Majorana masses with the TeV ...
In this paper we propose a possible explanation of the active neutrino Majorana masses with the TeV ...
If dark matter is light, it may be due to a seesaw mechanism just as neutrinos are. It is postulated...
We study a one-loop induced neutrino mass model with an inert isospin triplet scalar field of $Y=0$ ...
Searches for Dark Matter suggest that it couples to ordinary matter only very weakly and possibly on...
We show that the minimal Type-I Seesaw mechanism can successfully account for the observed dark matt...
We extend the Dirac Scotogenic model with the aim of realizing neutrino masses together with the mas...
The hierarchy in scale between atmospheric and solar neutrino mass splittings is investigated throug...
We present a three-loop model of neutrino mass whose most-general Lagrangian possesses a softly-brok...
We propose an extension of the standard model (SM) by including a dark sector comprised of three gen...
AbstractA new and radical scenario of the simple 2006 model of radiative neutrino mass is proposed, ...
We explore a gauged $U(1)_{B-L}$ extension of standard model with inclusion of three right-handed ne...
The scotogenic model presents an elegant and succinct framework for elucidating the origin of tiny n...
We discuss the impact of neutrino phenomenology and related cosmology on a $A_{4}\otimes Z_{8}$ symm...
The $SU(3)_c^{}\times SU(2)_L^{} \times U(1)_Y^{}$ standard model is extended by a $U(1)_{B-L}^{}$ g...
In this paper we propose a possible explanation of the active neutrino Majorana masses with the TeV ...
In this paper we propose a possible explanation of the active neutrino Majorana masses with the TeV ...