Abstract

An SO(10) model where the 10H and 120H representations are used for generating fermion masses is quite predictive, though due to the absence of SU(2)L,R triplet/singlet fields it cannot give rise to neutrino masses through the usual type-I or type-II seesaw mechanisms. In this Letter, for neutrino masses, we propose an extension of such an SO(10) model by adding fermions in the adjoint representation (45F) and a symmetry breaking scalar 16¯H. The 16¯H couples the adjoint fermions to the standard fermions in 16F and induces neutrino masses through the ‘double seesaw’ mechanism. In addition, we impose (i) a parity symmetry leading to hermitian Yukawa Matrices and (ii) a μ–τ flavor symmetry on the Yukawa matrices for 10H and 16¯H whereas for the 120H it is assumed to be antisymmetric. Thus we consider the model SO(10)⊗Z2(μ−τ)⊗Z2P. We discuss the conditions that the mass matrices must obey so that the model can reproduce the tri-bimaximal mixing pattern.

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