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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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