PHYS08200604017 Manimala Mitra - Homi Bhabha National Institute
PHYS08200604017 Manimala Mitra - Homi Bhabha National Institute
PHYS08200604017 Manimala Mitra - Homi Bhabha National Institute
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sector contains the exact/approximate Z 2 symmetry along the ν µ − ν τ direction, while<br />
it is broken down maximally in the charged lepton sector. This particular feature is<br />
achieved by the vacuum alignments of the different Higgs fields ∆, φ e and ξ. Exact<br />
µ−τ symmetry in the neutrino mass matrix is achieved as a consequence of the vacuum<br />
alignments 〈∆ 1 〉 = 〈∆ 2 〉 and 〈ξ 1 〉 = 〈ξ 2 〉, otherwise resulting in mildly broken µ − τ<br />
symmetry. The mild breaking of µ−τ symmetry opens up the possibility of CP violation<br />
in the leptonic sector. We have analyzed the potential and we show that under the<br />
most general case, the minimization condition predicts a very mild breaking of the µ−τ<br />
symmetry for the neutrinos. The charged lepton sector offers very tiny contribution to<br />
the physically observed PMNS mixing matrix, while the main contribution comes from<br />
the neutrino mixing matrix. In the neutrino sector both normal and inverted hierarchy<br />
are allowed possibilities.<br />
Since the Higgs triplet ∆ interacts with the gauge bosons via their kinetic terms,<br />
they can be produced at the LHC and then can be traced via their subsequent decays.<br />
The doubly charged Higgs can decay to different states such as dileptons, gauge bosons,<br />
singly charged Higgs H + . In our model the mixing between the two doubly charged Higgs<br />
is very closely related with the extent of the µ−τ symmetry in the neutrino sector. In<br />
the exact µ−τ limit the mixing angle θ between the two doubly charged Higgs is θ = π,<br />
4<br />
whereas mild breaking of the µ−τ symmetry results in a mild deviation θ ∼ π . This close<br />
4<br />
connection between the µ−τ symmetry and the doubly charged mixing angle significantly<br />
effects the doubly charged Higgs-dileptonic vertices. In the exact µ−τ limit, the vertex<br />
factors H 2 ++ −µ−τ and H 2 ++ −e−e are zero, hence the doubly charged Higgs H 2 ++ never<br />
decays to µ + +τ + or to 2e + states. Other than this, the non observation of the eµ and<br />
eτ states in the dileptonic decay of the doubly charged Higgs would possibly disfavor the<br />
inverted mass hierarchy of the standard model neutrino. The presence of Higgs triplet<br />
predicts lepton flavor violating processes such at τ → eeµ at the tree level. This and<br />
other lepton flavor violating processes could therefore be used to constrain the model as<br />
well as the neutrino mass hierarchy.<br />
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