AbstractFor type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass matrices are real and diagonal, four has been shown to be the maximum number of zeros allowed in the neutrino Yukawa coupling matrix Yν. These four zero textures have been classified into two distinct categories. We investigate certain phenomenological consequences of these textures within a supersymmetric framework. This is done by using conditions implied on elements of the neutrino Majorana mass matrix for textures of each category in Yν. These conditions turn out to be stable under radiative corrections. Including the effective mass, which appears in neutrinoless double beta decay, along with the usual neutrino masses, mixing angles ...
The generation of the right amount of baryon asymmetry η of the Universe from supersymmetric le...
We note that the emerging features of lepton mixing can be reproduced if, with inverted neutrino mas...
The consequences of a texture zero at the $ee$ entry of neutrino mass matrix in the flavor basis, wh...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
AbstractFor type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino ...
Within the type-I seesaw framework with three heavy right chiral neutrinos and in the basis where th...
We investigate, within the type I seesaw framework, the physical implications of zero textures in th...
We investigate, within the Type I seesaw framework, the physical implications of zero textures in th...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
The leptogenesis is studied in the neutrino mass matrix with two zeros, which reduces the number of ...
Four zero neutrino Yukawa textures in a specied weak basis, combined with μτ symmetry and type-I see...
We study the zero textures of the Yukawa matrices in the Minimal Extended type-I Seesaw (MES) model ...
AbstractWe study predictive textures for the lepton mass matrices in which the charged-lepton mass m...
AbstractThe leptogenesis is studied in the neutrino mass matrix with two zeros, which reduces the nu...
The generation of the right amount of baryon asymmetry η of the Universe from supersymmetric le...
We note that the emerging features of lepton mixing can be reproduced if, with inverted neutrino mas...
The consequences of a texture zero at the $ee$ entry of neutrino mass matrix in the flavor basis, wh...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
AbstractFor type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino ...
Within the type-I seesaw framework with three heavy right chiral neutrinos and in the basis where th...
We investigate, within the type I seesaw framework, the physical implications of zero textures in th...
We investigate, within the Type I seesaw framework, the physical implications of zero textures in th...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
For type I seesaw and in the basis where the charged lepton and heavy right-handed neutrino mass mat...
The leptogenesis is studied in the neutrino mass matrix with two zeros, which reduces the number of ...
Four zero neutrino Yukawa textures in a specied weak basis, combined with μτ symmetry and type-I see...
We study the zero textures of the Yukawa matrices in the Minimal Extended type-I Seesaw (MES) model ...
AbstractWe study predictive textures for the lepton mass matrices in which the charged-lepton mass m...
AbstractThe leptogenesis is studied in the neutrino mass matrix with two zeros, which reduces the nu...
The generation of the right amount of baryon asymmetry η of the Universe from supersymmetric le...
We note that the emerging features of lepton mixing can be reproduced if, with inverted neutrino mas...
The consequences of a texture zero at the $ee$ entry of neutrino mass matrix in the flavor basis, wh...