TY - JOUR
T1 - Cobimaximal lepton mixing from soft symmetry breaking
AU - Grimus, Walter
AU - Lavoura, Luis
N1 - Publisher Copyright:
© 2017 The Authors
PY - 2017/11/10
Y1 - 2017/11/10
N2 - Cobimaximal lepton mixing, i.e. θ23=45° and δ=±90° in the lepton mixing matrix V, arises as a consequence of SV=V⁎P, where S is the permutation matrix that interchanges the second and third rows of V and P is a diagonal matrix of phase factors. We prove that any such V may be written in the form V=URP, where U is any predefined unitary matrix satisfying SU=U⁎, R is an orthogonal, i.e. real, matrix, and P is a diagonal matrix satisfying P2=P. Using this theorem, we demonstrate the equivalence of two ways of constructing models for cobimaximal mixing—one way that uses a standard CP symmetry and a different way that uses a CP symmetry including μ–τ interchange. We also present two simple seesaw models to illustrate this equivalence; those models have, in addition to the CP symmetry, flavour symmetries broken softly by the Majorana mass terms of the right-handed neutrino singlets. Since each of the two models needs four scalar doublets, we investigate how to accommodate the Standard Model Higgs particle in them.
AB - Cobimaximal lepton mixing, i.e. θ23=45° and δ=±90° in the lepton mixing matrix V, arises as a consequence of SV=V⁎P, where S is the permutation matrix that interchanges the second and third rows of V and P is a diagonal matrix of phase factors. We prove that any such V may be written in the form V=URP, where U is any predefined unitary matrix satisfying SU=U⁎, R is an orthogonal, i.e. real, matrix, and P is a diagonal matrix satisfying P2=P. Using this theorem, we demonstrate the equivalence of two ways of constructing models for cobimaximal mixing—one way that uses a standard CP symmetry and a different way that uses a CP symmetry including μ–τ interchange. We also present two simple seesaw models to illustrate this equivalence; those models have, in addition to the CP symmetry, flavour symmetries broken softly by the Majorana mass terms of the right-handed neutrino singlets. Since each of the two models needs four scalar doublets, we investigate how to accommodate the Standard Model Higgs particle in them.
KW - NEUTRINO MASS
UR - https://arxiv.org/abs/1708.09809
UR - https://www.scopus.com/pages/publications/85033600359
U2 - 10.1016/j.physletb.2017.09.082
DO - 10.1016/j.physletb.2017.09.082
M3 - Article
SN - 0370-2693
VL - 774
SP - 325
EP - 331
JO - Physics Letters. Section B: Nuclear, Elementary Particle and High-Energy Physics
JF - Physics Letters. Section B: Nuclear, Elementary Particle and High-Energy Physics
ER -