Abstract We study the contributions of supersymmetric models with a U(1) horizontal symmetry and only spontaneous CP breaking to various lepton flavor observables, such as μ → eγ and the electron electric dipole moment. We show that both a horizontal symmetry and a lack of explicit CP violation can alleviate the existing bounds from such observables. The undetermined O $$ \mathcal{O} $$ (1) coefficients in such mass matrix models muddle the interpretation of the bounds from various flavor observables. To overcome this, we define a new fine-tuning measure for different observables in such setups. This allows us to study how naturally the observed IR flavor observables can emerge from a given mass matrix model. We use our flavor-naturalness m...
A non-Abelian flavour symmetry in a minimal supersymmetric standard model can explain the flavour st...
Spontaneous breaking of inter-family (horizontal) gauge symmetries can be at the origin of the mass ...
Abstract We study the phenomenology of a unified supersymmetric theory with a flavor symmetry Δ(27)....
Abstract We study the contributions of supersymmetric models w...
Abstract Hierarchical masses of quarks and leptons are addressed by imposing horizontal symmetries. ...
We analyze the phenomenological consequences of embedding a flavor symmetry based on the groups A an...
Abstract The electric dipole moment (EDM) of electron is studied in the supersymmetric A4 modular in...
The muon g−2 anomaly is a long-standing discrepancy from its standard model prediction. The recent i...
AbstractA supersymmetric see-saw model obeying the flavor symmetry Lμ−Lτ, which naturally predicts q...
In this paper, we present a model which employs CP × Z3 symmetries where quark mixing and charged le...
Assuming that the lepton, quark and Higgs fields belong to the three-dimensional re-ducible represen...
The heaviness of the third family fermions and the experimental absence of large flavor violating pr...
AbstractCurrent data from neutrino oscillation experiments are in good agreement with δ=−π2 and θ23=...
The smallness of the quark sector parameters and the hierarchy between them could be the result of a...
We consider lepton flavor violations (LFV) mediated by photino as a result of the nondiagonal slepto...
A non-Abelian flavour symmetry in a minimal supersymmetric standard model can explain the flavour st...
Spontaneous breaking of inter-family (horizontal) gauge symmetries can be at the origin of the mass ...
Abstract We study the phenomenology of a unified supersymmetric theory with a flavor symmetry Δ(27)....
Abstract We study the contributions of supersymmetric models w...
Abstract Hierarchical masses of quarks and leptons are addressed by imposing horizontal symmetries. ...
We analyze the phenomenological consequences of embedding a flavor symmetry based on the groups A an...
Abstract The electric dipole moment (EDM) of electron is studied in the supersymmetric A4 modular in...
The muon g−2 anomaly is a long-standing discrepancy from its standard model prediction. The recent i...
AbstractA supersymmetric see-saw model obeying the flavor symmetry Lμ−Lτ, which naturally predicts q...
In this paper, we present a model which employs CP × Z3 symmetries where quark mixing and charged le...
Assuming that the lepton, quark and Higgs fields belong to the three-dimensional re-ducible represen...
The heaviness of the third family fermions and the experimental absence of large flavor violating pr...
AbstractCurrent data from neutrino oscillation experiments are in good agreement with δ=−π2 and θ23=...
The smallness of the quark sector parameters and the hierarchy between them could be the result of a...
We consider lepton flavor violations (LFV) mediated by photino as a result of the nondiagonal slepto...
A non-Abelian flavour symmetry in a minimal supersymmetric standard model can explain the flavour st...
Spontaneous breaking of inter-family (horizontal) gauge symmetries can be at the origin of the mass ...
Abstract We study the phenomenology of a unified supersymmetric theory with a flavor symmetry Δ(27)....