arXiv subjects

Shankita Bhardwaj

Publications and source records attributed to Shankita Bhardwaj.

5 recordsLinked to original sources

arXiv2020

Non-Standard Interactions and Prospects for Studying Standard Parameter Degeneracies in DUNE and T2HKK

The future long baseline experiments such as DUNE and T2HKK have promising prospects to determine the neutrino mass hierarchy and measuring standard $CP$ phase $δ$. However, presence of possible non-standard interactions of neutrinos with matter may intricate this picture and is the subject matter of the present work. We have studied the standard parameter degeneracies in presence of non-standard interactions(NSI) with DUNE and T2HKK experiments. We examine the mass hierarchy degeneracy assuming (i) all NSI parameters to be non-zero and (ii) one NSI parameter($ε_{eμ}$) and its corresponding $CP$ phase($δ_{eμ}$) to be non-zero. We find that the later case is more appropriate to resolve mass hierarchy degeneracy with DUNE and T2HKK experiments due to relatively small uncertainties emanating from the NSI sector. We have, also, investigated the octant degeneracy with neutrino($ν_μ\rightarrowν_{e}$) and antineutrino($\barν_μ\rightarrow\barν_{e}$) mode separately. We find that to resolve this degeneracy the long baseline experiment with combination of neutrino and antineutrino mode is essential. Furthermore, we have considered DUNE in conjunction with T2HKK experiment to study $CP$ phase degeneracy due to standard($δ$) and non-standard($δ_{eμ}$) $CP$ phases. We find that DUNE and T2HKK, in conjunction, has more sensitivity for $CP$ violation effects(10$σ$ for true NH and 8.2$σ$ for true IH).

hep-ph↗

arXiv2019

Highly predictive and testable $A_{4}$ flavor model within type-I and II seesaw framework and associated phenomenology

We investigate neutrino mass model based on $A_4$ discrete flavor symmetry in type-I+II seesaw framework. The model has imperative predictions for neutrino masses, mixing and $CP$ violation testable in the current and upcoming neutrino oscillation experiments. The important predictions of the model are: normal hierarchy for neutrino masses, a higher octant for atmospheric angle ($θ_{23}>45^{o}$) and near-maximal Dirac-type $CP$ phase ($δ\approxπ/2$ or $3π/2$) at $3σ$ C. L.. These predictions are in consonance with the latest global-fit and results from Super-Kamiokande(SK), NO$ν$A and T2K. Also, one of the important feature of the model is the existence of a lower bound on effective Majorana mass, $|M_{ee}|\geq 0.047$eV(at 3$σ$) which corresponds to the lower part of the degenerate spectrum and is within the sensitivity reach of the neutrinoless double beta decay(0$νββ$) experiments.

hep-ph↗

arXiv2018

Quark-lepton complementarity model based predictions for $θ_{23}^{PMNS}$ with neutrino mass hierarchy

After the successful investigation and confirmation of non zero $θ_{13}^{PMNS}$ by various experiments, we are standing at a square where we still encounter a number of issues, which are to be settled. In this paper, we have extended our recent work towards a precise prediction of the $θ_{23}^{PMNS}$ mixing angle, taking into account the neutrino mass hierarchy. We parameterize the non-trivial correlation between quark (CKM) and lepton (PMNS) mixing matrices in quark-lepton complementarity (QLC) model as $V_{c}= U_{CKM}. ψ. U_{PMNS}$, where $ψ$ is a diagonal phase matrix. Monte Carlo simulations are used to estimate the texture of $V_{c}$ and compare the results with the standard Tri-Bi-Maximal (TBM) and Bi-Maximal(BM) structures of neutrino mixing matrix. We have predicted the value of $θ_{23}^{PMNS} $ for normal and inverted neutrino mass hierarchies. The value of $θ_{23}^{PMNS}$ obtained for two cases are about $1.3σ$ away from each other, implying the better precision can give us a strong hint for the type of neutrino mass hierarchy.

hep-ph↗

arXiv2016

Probing Non-unitary $CP$ Violation effects in Neutrino Oscillation Experiments

In the present work, we have considered minimal unitarity violation(MUV) scheme, to obtain the general expression for $ν_μ\rightarrowν_τ$ oscillation probability, in vacuum. For this channel, we have investigated the sensitivities to non-unitary parameters $|ρ_{μτ}|$ and $ω_{μτ}$ with short baseline(SBL) experiments for normal as well as inverted hierarchical neutrino masses. We also check how the sensitivity to non-unitary parameters get modified for $θ_{23}$ above and below maximality. We find that the $3σ$ sensitivity towards $|ρ_{μτ}|$ is maximum for non-unitary phase $ω_{μτ}=0$, whereas it is minimum for $ω_{μτ}=\pmπ$ in case of normal hierarchy(NH). However, the sensitivity is minimum at $ω_{μτ}=0$ and maximum for $ω_{μτ}=\pmπ$ for inverted hierarchy(IH). We observe that for unitary $CP$ phase $δ=0$ and $δ=π/2$, the sensitivity to measure non-unitarity remains same in both the cases. We, also, explore wide range of $L/E$ to forecast, in principle, the possibilities to observe $CP$-violation due to unitary($δ$) and non-unitary($ω_{μτ}$) phases. We find that the both phases can be disentangled, in principle, from each other, for the $L/E$ range less than 200 km/GeV for $ν_μ\rightarrowν_τ$ channel.

hep-ph↗

arXiv2016

Prospects for Reconstruction of Leptonic Unitarity Quadrangle and Neutrino Oscillation Experiments

After the observation of non-zero $θ_{13}$ the goal has shifted to observe $CP$ violation in the leptonic sector. Neutrino oscillation experiments can, directly, probe the Dirac $CP$ phases. Alternatively, one can measure $CP$ violation in the leptonic sector using Leptonic Unitarity Quadrangle(LUQ). The existence of Standard Model (SM) gauge singlets - sterile neutrinos - will provide additional sources of $CP$ violation. We investigate the connection between neutrino survival probability and rephasing invariants of the $4\times4$ neutrino mixing matrix. In general, LUQ contain eight geometrical parameters out of which five are independent. We obtain $CP$ asymmetry($P_{ν_f\rightarrowν_{f'}}-P_{\barν_f\rightarrow\barν_{f'}}$) in terms of these independent parameters of the LUQ and search for the possibilities of extracting information on these independent geometrical parameters in short baseline(SBL) and long baseline(LBL) experiments, thus, looking for constructing LUQ and possible measurement of $CP$ violation. We find that it is not possible to construct LUQ using data from LBL experiments because $CP$ asymmetry is sensitive to only three of the five independent parameters of LUQ. However, for SBL experiments, $CP$ asymmetry is found to be sensitive to all five independent parameters making it possible to construct LUQ and measure $CP$ violation.

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