Abstract

Dominance of type-II seesaw mechanism for neutrino masses has attracted considerable attention because of a number of advantages. We show a novel approach to achieve Type-II seesaw dominance in non-supersymmetric $SO(10)$ grand unification where a low mass $Z^{\prime}$ boson and specific patterns of right-handed neutrino masses are predicted within the accessible energy range of the Large Hadron Collider. In spite of the high value of the seesaw scale, $M_{\Delta_L} \simeq 10^8-10^9$ GeV, the model predicts new dominant contributions to neutrino-less double beta decay in the $W_L-W_L$ channel close to the current experimental limits via exchanges of heavier singlet fermions used as essential ingredients of this model even when the light active neutrino masses are normally hierarchical or invertedly hierarchical. We obtain upper bounds on the lightest sterile neutrino mass $m_s\lesssim 3.0$ GeV, $2.0$ GeV, and $0.7$ GeV for normally hierarchical, invertedly hierarchical, and quasi-degenerate patterns of light neutrino masses, respectively. The underlying non-unitarity effects lead to lepton flavor violating decay branching ratios within the reach of ongoing or planned experiments and the leptonic CP-violation parameter nearly two orders larger than the quark sector. Some of the predicted values on proton lifetime for $p\to e^+\pi^0$ are found to be within the currently accessible search limits. Other aspects of model applications including leptogenesis etc. are briefly indicated.

Highlights

  • Mν = m I ν I + mνI, (1) −MD MDT, (2) f vL (3)

  • Scale vacuum expectation value (VEV) of VR, the Type-II seesaw mechanism predicts RH neutrino masses which can be testified at the Large Hadron Collider (LHC) or future high energy accelerators

  • We derive an analytic formula for the half-life of 0νββ decay as a function of the singlet fermion masses, predicting a lower bound on the lightest sterile neutrino mass eigenvalue from the current experimental data on the lower bounds

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Summary

Introduction

Where MD(MN ) is the Dirac (RH-Majorana) neutrino mass, vL is the induced vacuum expectation value (VEV) of the left-handed (LH) triplet L , and f is the Yukawa coupling of the triplet. Two-step breakings of LR gauge theory was embedded earlier in non-SUSY GUTs with low-mass Z (for earlier work on, Z boson in GUTs embedding two-step breaking of left-right gauge symmetry, see [33,34,35]), its successful compliance with neutrino oscillation data has been possible in the context of an inverse seesaw mechanism [36]. Compared to earlier existing SO(10)-based Type-II seesaw dominant models whose RH neutrino masses are in the inaccessible range and new gauge bosons are in the mass range 1015–1017 GeV, the present model predictions on LHC scale Z , light and heavy Majorana type sterile neutrinos, RH Majorana neutrino masses in the range 100–10, 000 GeV accessible to LHC in the WL − WL channel through dilepton production, the LFV branching ratios closer to experimental limits, and dominant 0νββ decay amplitudes caused by sterile neutrino exchanges provide a rich testing ground for new physics signatures.

Unification with TeV scale Z
Renormalisation group solutions to mass scales
10 TeV for
Proton-lifetime prediction
Derivation of Type-II seesaw formula
Suppression of linear seesaw and dominance of Type-II seesaw
Right-handed neutrino mass prediction
The Dirac neutrino mass matrix
Extrapolation to the GUT-scale
Lepton flavour violation
Estimation of non-unitarity matrix
Branching ratio and CP violation
Neutrino-less double beta decay
Effective mass parameter and half-life
Numerical estimations of effective mass parameters
Cancellation between effective mass parameters
Half-life as a function of singlet fermion masses
Electroweak precision observables and other constraints
Brief discussion of other aspects and leptogenesis
Possibility of dilepton signals at LHC
Leptogenesis
Summary and conclusion
11.1 Block diagonalisation and determination of Mν
11.4 Determination of Q2
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