Searcharxiv⌕ Search

arXiv subjects

S. Robertson Singh

Publications and source records attributed to S. Robertson Singh.

4 recordsLinked to original sources

Modular $A_4$ symmetry in 3+1 active-sterile neutrino masses and mixings

Motivated by the significance of modular symmetry in generating neutrino masses and flavor mixings, we apply the modular $A_4$ symmetry in a 3+1 scheme of active-sterile neutrino mixings. Neutrino oscillation observables in the 3$σ$ range are successfully reproduced through the vacuum expectation value of the modulus $τ$. We also study phenomenologies related to the effective neutrino masses $m_β$ in tritium beta decay and $m_{ββ}$ in neutrinoless double beta decay. Mixings between active neutrinos and eV scale sterile neutrino are analyzed in detail. The model also predicts the Dirac CP-violating phase $δ_{CP}$ and Majonara phases $α$ and $β$. The best-fit values of the neutrino mixing angles and ratios of two mass-squared differences are determined using minimum $χ^2$ analysis. The best-fit values of the neutrino oscillation observables are predicted as $\sin^2θ_{23}=0.573,$ $\sin^2θ_{12}=0.300,$ $ \sin^2θ_{13}=0.022$ and $r = 0.172$ for NH while $\sin^2θ_{23}=0.550,$ $\sin^2θ_{12}=0.303,$ $ \sin^2θ_{13}=0.022$ and $r = 0.171$ for IH. We also observe that the predictions of effective neutrino mass parameters in the 3+1 scheme are significantly different from the three neutrino paradigm.

hep-ph↗

KeV dark matter in minimal extended seesaw model and its predictions in neutrinoless double beta decay and baryogenesis

We develop an $A_4 \times Z_4 \times Z_2$ symmetry extension of Standard Model under the minimal extended seesaw (MES) mechanism which successfully predicts neutrino masses and mixings patterns. This model breaks $μ-τ$ symmetry of neutrino mass matrix and explains leptonic mixing with non-zero $θ_{13}$. We study the phenomenological results of the keV-scale sterile neutrino as a dark matter candidate along with other phenomenologies such as neutrino oscillation observables, neutrinoless double beta decay, baryogenesis via leptogenesis, etc. Dirac CP-violating phase $δ_{CP}$ and two Majorana phases $α$ and $β$ are also calculated from the leptonic mixing matrix. Best-fit values of the model parameters and neutrino observables are calculated from $χ^2$ analysis. The model predicts best-fit values of neutrino mixing angles to be $\sin^2θ_{23}=0.555,\ \sin^2θ_{12}=0.301$ and $\sin^2θ_{13}=0.022$ for normal hierarchy. Significant results consistent with experimental data are also observed for effective neutrino mass $m_{ββ} \sim (0.97 - 5.02)$ meV, effective electron mass $m_β \sim (0.084-0.41)$eV and sum of active neutrino masses $\sum m_{i} < 0.12$ eV. The model does not favour Inverted hierarchy at the 3$σ$ level with the given parameter space.

hep-ph↗

Deviation from Tribimaximal mixing using $A_{4}$ flavour model with five extra scalars

A modified neutrino mass model with five extra scalars is constructed using $A_{4}$ discrete symmetry group. The resultant mass matrix is able to give necessary deviation from Tribimaximal mixing which reproduces the current neutrino masses and mixing data with good accuracy. The model gives testable prediction for the future measurements of the neutrinoless double-beta decay parameter $|m_{ββ}|$. The analysis is consistent with latest cosmological bound $Σm_{i}\leq$ 0.12 eV.

hep-ph↗

Active-Sterile neutrino masses and mixings in $A_4$ minimal extended seesaw mechanism

Assuming the existence of an eV or KeV scale sterile neutrino, we develop a 3+1 neutrino mass model using $A_4\times Z_4 \times Z_2$ symmetry group. Three Higgs $H, H^{\prime}$ and $H^{\prime\prime}$ are considered to give a desired neutrino mass matrix which generates non-zero $θ_{13}$. The model can give neutrino mixing parameters that are well within the experimental 3$σ$ bounds. We also calculate the $4\times 4$ active-sterile neutrino mixing matrix, and it is found to be consistent with experimental bounds.

hep-ph↗