47 research outputs found

    Neutrino Mixing Phenomenology: A4A_4 Discrete Flavor Symmetry with Type-I Seesaw Mechanism

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    We study a neutrino mass model with A4A_4 flavor symmetry using a type-I seesaw mechanism. The inclusion of extra flavons in our model leads to the deviations from exact tribimaximal mixing pattern resulting in a nonzero θ13\theta_{13} consistent with the recent experimental results and a sum rule for light neutrino masses is also obtained. In this framework, a connection is established among the mixing angles (θ13\theta_{13}, θ12\theta_{12}, θ13\theta_{13}) and the Dirac CP-violation phase δCP\delta_{CP}. This model also allows us a prediction of Jarlskog parameter JCPJ_{CP} and the octant of the mixing angle θ23\theta_{23}. We use the parameter space of our model of neutrino masses to study the neutrinoless double beta decay parameter meem_{ee}.Comment: 15 pages, 3 Figures, 2 Table

    Double Stage chain routing Protocal in WSN

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    Wireless sensor networking is most popular fields in today’s world. In this paper, we have discussed the different energy optimization protocols of WSN. We have forwarded a new protocol “Double Stage Chain Routing Protocol†from WSN. Our main focus is on extending the residual energy and network’s life time at least more than LEACH, CCM and TSCP. The result of our protocol is represented with the help of graph with comparison with TSCP and it is found that DSCRP gives better network lifetime than LEACH. The proposed algorithm is acceptable in the network lifetime of DSCRP as well as in network life time

    Non-zero θ13\theta_{13}, CP-violation and Neutrinoless Double Beta Decay for Neutrino Mixing in the A4×Z2×Z2A_4\times Z_2\times Z_2^\prime Flavor Symmetry Model

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    We study the modification of the Altarelli-Feruglio A4A_4 flavor symmetry model by adding three singlet flavons ξ\xi', ξ\xi'' and ρ\rho and the model is augmented with extra Z2×Z2Z_2\times Z_2^ \prime symmetry to prevent the unwanted terms in our study. The addition of these three flavons lead to two higher order corrections in the form of two perturbation parameters ϵ\epsilon and ϵ\epsilon^\prime. These corrections yield the deviation from exact tri-bimaximal (TBM) neutrino mixing pattern by producing a non-zero θ13\theta_{13} and other neutrino oscillation parameters which are consistent with the latest experimental data. In both the corrections, the neutrino masses are generated via Weinberg operator. The analysis of the perturbation parameters ϵ\epsilon and ϵ\epsilon^\prime, shows that normal hierarchy (NH) and inverted hierarchy (IH) for ϵ\epsilon does not change much. However, as the values of ϵ\epsilon^\prime increases, θ23\theta_{23} occupies the lower octant for NH case. We further investigate the neutrinoless double beta decay parmeter mββm_{\beta\beta} using the parameter space of the model for both normal and inverted hierarchies of neutrino masses.Comment: 19 pages, 6 figures, 3 table

    Neutrino Mass Model in the Context of Δ(54)Z2Z3Z4\boldsymbol{\Delta(54) \otimes Z_2\otimes Z_3 \otimes Z_4} Flavor Symmetries with Inverse Seesaw Mechanism

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    Our analysis involves enhancing the Δ(54)\Delta(54) flavor symmetry model with Inverse Seesaw mechanism along with two SM Higgs through the incorporation of distinct flavons. Additionally, we introduce supplementary Z2Z3Z4Z_2\otimes Z_3 \otimes Z_4 symmetries to eliminate any undesirable components within our investigation. The exact tri-bimaximal neutrino mixing pattern undergoes a deviation as a result of the incorporation of extra flavons, leading to the emergence of a non-zero reactor angle θ13\theta_{13} that aligns with the latest experimental findings. It was found that for our model the atmospheric oscillation parameter occupies the lower octant for normal hierarchy case. We also examine the parameter space of the model for normal hierarchy to explore the Dirac CP (δCP\delta_{CP}), Jarlskog invariant parameter (JJ) and the Neutrinoless double-beta decay parameter (mββm_{\beta\beta}) and found it in agreement with the neutrino latest data. Hence our model may be testable in the future neutrino experiments.Comment: 18 pages, 6 figures, 3 table
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