In the type I + II seesaw formula the mass matrix of light neutrinos m_nu receives contributions from the exchanges of both heavy Majorana neutrinos and SU(2)_L-triplet Higgs bosons. We propose a new parameterization for the Dirac-type Yukawa coupling matrix of neutrinos in this case, which generalizes the well known Casas-Ibarra parameterization to type I + II seesaw and is useful when the triplet term in m_nu is known. Neutrino masses and mixing, lepton flavor violation in decays like mu -> e \gamma within mSUGRA models and leptogenesis can then be studied within this framework. We illustrate the usefulness of our new parameterization using a number of simple examples
We introduce three right-handed neutrinos and three sterile neutrinos, and consider an inverse seesa...
In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the ex...
AbstractFor type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino ...
A see-saw mechanism for the masses of the light active neutrinos and their mixing angles is proposed...
We discuss symmetries and scenarios leading to quasi-degenerate neutrinos in type I seesaw models. T...
A mechanism has been suggested recently to generate the neutrino mass out of a dimension-seven opera...
In the context of Standard Model (SM) extensions, the seesaw mechanism provides the most natural exp...
We consider type I+II seesaw mechanism, where the exchanges of both right-handed neutrinos and isotr...
We discuss what kinds of combinations of Yukawa interactions can generate the Majorana neutrino mass...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
Abstract We discuss how seesaw neutrino models can be graphically represented in lepton flavour spac...
AbstractWe discuss what kinds of combinations of Yukawa interactions can generate the Majorana neutr...
We discuss the phenomenology of type-II seesaw by extending the standard model with additional Higgs...
We consider a version of the low-scale type I seesaw mechanism for generating small neutrino masses,...
The origin of tiny neutrino masses and the baryon number asymmetry of the Universe are naturally int...
We introduce three right-handed neutrinos and three sterile neutrinos, and consider an inverse seesa...
In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the ex...
AbstractFor type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino ...
A see-saw mechanism for the masses of the light active neutrinos and their mixing angles is proposed...
We discuss symmetries and scenarios leading to quasi-degenerate neutrinos in type I seesaw models. T...
A mechanism has been suggested recently to generate the neutrino mass out of a dimension-seven opera...
In the context of Standard Model (SM) extensions, the seesaw mechanism provides the most natural exp...
We consider type I+II seesaw mechanism, where the exchanges of both right-handed neutrinos and isotr...
We discuss what kinds of combinations of Yukawa interactions can generate the Majorana neutrino mass...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
Abstract We discuss how seesaw neutrino models can be graphically represented in lepton flavour spac...
AbstractWe discuss what kinds of combinations of Yukawa interactions can generate the Majorana neutr...
We discuss the phenomenology of type-II seesaw by extending the standard model with additional Higgs...
We consider a version of the low-scale type I seesaw mechanism for generating small neutrino masses,...
The origin of tiny neutrino masses and the baryon number asymmetry of the Universe are naturally int...
We introduce three right-handed neutrinos and three sterile neutrinos, and consider an inverse seesa...
In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the ex...
AbstractFor type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino ...