AbstractA scenario is proposed for bi-large lepton mixing in the framework of nearly threefold degenerate Majorana neutrinos. In our proposal, we impose Z3 symmetry in the neutrino sector at a high energy scale to account for the threefold degenerate neutrinos and the maximal mixing between νμ and ντ. In order to obtain the atmospheric neutrino mass splitting while keeping the maximal mixing between νμ and ντ, we introduce a small perturbation to the neutrino mass matrix without breaking Z3 symmetry. On the other hand, the solar neutrino mixing arises due to the non-diagonal charged lepton mass matrix, and the desirable large mixing and mass splitting for the solar neutrino oscillation can be obtained by radiative corrections
AbstractWe find that the presence of a global Le−Lμ−Lτ (≡L′) symmetry and an S2 permutation symmetry...
We investigate in a model-independent way to what extent one can perturb tri-bimaximal mixing in ord...
We take up the point of view that Yukawa couplings can be either 0 or 1, and the mass patterns of fe...
AbstractA scenario is proposed for bi-large lepton mixing in the framework of nearly threefold degen...
The neutrino mixing matrix U is in general of the form , where Ue arises from the diagonalization of...
We present a model for leptonic mixing and the lepton masses based on flavor symmetries and higher-d...
It is well-known that, in the basis where the charged-lepton mass matrix is diagonal, there are seve...
AbstractIt is well known that, in the basis where the charged-lepton mass matrix is diagonal, there ...
AbstractWe propose a scenario that the mass splitting between the first generation of the heavy Majo...
I review the construction of a model for lepton masses based on the flavour symmetry group A4 x U(1)...
One of the outstanding problems in particle physics is the understanding of the origin of the fermio...
The mass matrix of three Majorana neutrinos of equal mass is not necessarily proportional to the ide...
We introduce a simple flavor symmetry breaking scheme, in which charged lepton masses have a strong ...
We propose that the observed large leptonic mixing may just reflect a quasidegeneracy of three Ma-jo...
We present a systematic study on minimally perturbed neutrino mass matrices which at the leading ord...
AbstractWe find that the presence of a global Le−Lμ−Lτ (≡L′) symmetry and an S2 permutation symmetry...
We investigate in a model-independent way to what extent one can perturb tri-bimaximal mixing in ord...
We take up the point of view that Yukawa couplings can be either 0 or 1, and the mass patterns of fe...
AbstractA scenario is proposed for bi-large lepton mixing in the framework of nearly threefold degen...
The neutrino mixing matrix U is in general of the form , where Ue arises from the diagonalization of...
We present a model for leptonic mixing and the lepton masses based on flavor symmetries and higher-d...
It is well-known that, in the basis where the charged-lepton mass matrix is diagonal, there are seve...
AbstractIt is well known that, in the basis where the charged-lepton mass matrix is diagonal, there ...
AbstractWe propose a scenario that the mass splitting between the first generation of the heavy Majo...
I review the construction of a model for lepton masses based on the flavour symmetry group A4 x U(1)...
One of the outstanding problems in particle physics is the understanding of the origin of the fermio...
The mass matrix of three Majorana neutrinos of equal mass is not necessarily proportional to the ide...
We introduce a simple flavor symmetry breaking scheme, in which charged lepton masses have a strong ...
We propose that the observed large leptonic mixing may just reflect a quasidegeneracy of three Ma-jo...
We present a systematic study on minimally perturbed neutrino mass matrices which at the leading ord...
AbstractWe find that the presence of a global Le−Lμ−Lτ (≡L′) symmetry and an S2 permutation symmetry...
We investigate in a model-independent way to what extent one can perturb tri-bimaximal mixing in ord...
We take up the point of view that Yukawa couplings can be either 0 or 1, and the mass patterns of fe...