We present an argument in which the scale \sim 0.1 eV associated with neutrino masses appears in a natural way from a class of (very) large volume compactifications, being tied to a supersymmetry scale of 10^3 GeV and a string scale of 10^{11} GeV. The masses are of Majorana type and there is no need for a see-saw mechanism. The suppression scale arises from a combination of TeV supersymmetry and locality of the Yukawa couplings. These kind of constructions appear naturally in Type IIB flux compactifications. However, the arguments that lead to this result rely only on a few geometrical features of the compactification manifold, and hence can be used independently of string theory
We show that in theories that reduce, at the Fermi scale, to an extension of the standard model with...
A small neutrino Majorana mass can arise in the Standard Model as an effective dimension 5 operator....
Recently it was proposed that the standard model (SM) degrees of freedom reside on a $(3+1)$-dimensi...
We present an argument in which the scale ~ 0.1 eV associated with neutrino masses naturally appears...
We discuss the profile of neutrino masses and mixings in models with large extra dimensions when rig...
We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upp...
We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upp...
We show that under a new U(1) gauge symmetry, which is non-anomalous in the presence of one ``right-...
We show that under a new U(1) gauge symmetry, which is non-anomalous in the presence of one ''right-...
Starting from a complete set of possible parametrisations of the quark-mass matrices that have the m...
The possibility of generating neutrino mass through see-saw mechanism involving U(1) chiral Peccei-Q...
Among three typical energy scales, a neutrino mass scale (mν∼0.1 eV), a GUT scale (MGUT∼1016 GeV), a...
It is shown that the Majorana nature of the heavy neutrinos $N_j$ having masses in the range of ...
AbstractIf the origin of neutrino masses is due to physics at the TeV scale, it would be of tremendo...
The possible existence of bulk singlet neutrinos in the scenario with large compactified dimensions ...
We show that in theories that reduce, at the Fermi scale, to an extension of the standard model with...
A small neutrino Majorana mass can arise in the Standard Model as an effective dimension 5 operator....
Recently it was proposed that the standard model (SM) degrees of freedom reside on a $(3+1)$-dimensi...
We present an argument in which the scale ~ 0.1 eV associated with neutrino masses naturally appears...
We discuss the profile of neutrino masses and mixings in models with large extra dimensions when rig...
We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upp...
We derive a model-independent upper bound on the scale of Majorana-neutrino mass generation. The upp...
We show that under a new U(1) gauge symmetry, which is non-anomalous in the presence of one ``right-...
We show that under a new U(1) gauge symmetry, which is non-anomalous in the presence of one ''right-...
Starting from a complete set of possible parametrisations of the quark-mass matrices that have the m...
The possibility of generating neutrino mass through see-saw mechanism involving U(1) chiral Peccei-Q...
Among three typical energy scales, a neutrino mass scale (mν∼0.1 eV), a GUT scale (MGUT∼1016 GeV), a...
It is shown that the Majorana nature of the heavy neutrinos $N_j$ having masses in the range of ...
AbstractIf the origin of neutrino masses is due to physics at the TeV scale, it would be of tremendo...
The possible existence of bulk singlet neutrinos in the scenario with large compactified dimensions ...
We show that in theories that reduce, at the Fermi scale, to an extension of the standard model with...
A small neutrino Majorana mass can arise in the Standard Model as an effective dimension 5 operator....
Recently it was proposed that the standard model (SM) degrees of freedom reside on a $(3+1)$-dimensi...