We propose a scotogenic scenario where the singlet-doublet dark matter plays an important role in generating Dirac neutrino mass. It is possible to address muon anomalous magnetic moment with charged doublet in the lo...
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We propose a scotogenic scenario where the singlet-doublet dark matter plays an important role in generating Dirac neutrino mass. It is possible to address muon anomalous magnetic moment with charged doublet in the loop. Due to the Dirac nature of neutrino, the additional right-handed neutrino (RHN) can contribute to the additional relativistic degrees of freedom, Delta Neff, in the Universe. We show that the tiny Dirac neutrino mass correlates the parameter space of muon (g - 2), Delta Neff and plays a non-trivial role in deciding the relic density of dark matter. We analyse the thermal dark matter and its detection prospects. We also explored thermal and non-thermal origin of Delta Neff and the parameter space, explored in this work, is verifiable at future CMB experiments like CMB-S4 and SPT-3G.
We develop a neutrino mass model based on Delta(27) discrete symmetry by using three Higgs doublets, three right-handed neutrinos, and two Delta(27) triplets to explain neutrino oscillation parameters consistent with ...
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We develop a neutrino mass model based on Delta(27) discrete symmetry by using three Higgs doublets, three right-handed neutrinos, and two Delta(27) triplets to explain neutrino oscillation parameters consistent with the Planck cosmological bound on the sum of the three absolute neutrino mass eigenvalues,. Sigma|m(i) | < 0.12 eV. The detailed numerical analysis is carried out by applying input model parameters and the predicted neutrino oscillation parameters are in agreement with the global neutrino oscillation data for both normal (NH) and inverted (IH) hierarchical model. We also calculate the effective neutrino masses for neutrinoless double beta decay (m(ee)), tritium beta decay (m beta), and Jarlskog invariant (J(CP)) for CP violation as m(ee) <= 30.6 meV,.m beta <= 30.5 meV, and J(CP) <= 0.0217 for NH, and m(ee) <= 51.7 meV, m beta <= 51.4 meV, and J(CP) <= 0.0222 for IH.
We explore the potential for low-scale leptogenesis in the singlet-triplet scotogenic model where dark matter participates in neutrino mass generation radiatively. Our investigation focuses on two possible scenarios. ...
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We explore the potential for low-scale leptogenesis in the singlet-triplet scotogenic model where dark matter participates in neutrino mass generation radiatively. Our investigation focuses on two possible scenarios. The first scenario introduces two heavy right-handed (RH) fermion fields, F and Sigma, with moderate hierarchy. In this case, the out-of-equilibrium decay of these particles results in the emergence of a lepton asymmetry. Our analysis reveals that the scale of leptogenesis in this scenario resembles that of standard thermal leptogenesis with. M-F,(Sigma) similar to 10(9) GeV. In the second scenario, we propose a framework to lower the scale of leptogenesis. In particular, we have considered two singlet fermions (F-1, F-2) and one triplet fermion (Sigma), which results in non-zero lightest active neutrino mass, i.e. m(1) not equal 0. With the mass hierarchy. M-F1 < M-Sigma << M-F2, this scenario yields a lower bound on heavy RH fermion, significantly reducing the scale of leptogenesis up to the TeV range. Also, real component of the neutral part of inert scalar (eta) is the dark matter candidate in the model.
We study the impact of invisible neutrino decay in the measurements of octant and mass hierarchy sensitivities at long-baseline neutrino experiments. DUNE (Deep Underground Neutrino Experiment) and T2HKK (Tokai-to-Hyp...
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We study the impact of invisible neutrino decay in the measurements of octant and mass hierarchy sensitivities at long-baseline neutrino experiments. DUNE (Deep Underground Neutrino Experiment) and T2HKK (Tokai-to-Hyper-Kamiokande-to-Korea) are two upcoming long baseline experiments that can contribute a lot to precision measurements in the neutrino sector. Assuming v(3) to be unstable, we show the effect of the invisible neutrino decay in the measurements of the sensitivities at the far detector of these experiments. We have also performed a combined analysis of the two experiments. The octant sensitivity increases, while mass hierarchy sensitivity changes very slightly in the presence of invisible neutrino decay. The value of the decay parameter. tau(3)/m(3) considered in this work is 2.2 x 10(-11) s/eV.
In the multi-component dark matter (DM) framework, DM-DM conversion has an important role in DM phenomenology. Depending on its conversion rate and its visible connection, we might be able to reach different kinds of ...
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In the multi-component dark matter (DM) framework, DM-DM conversion has an important role in DM phenomenology. Depending on its conversion rate and its visible connection, we might be able to reach different kinds of multipartite thermal DM scenarios. Here, we show the dynamics of DM.(DM1), which has a feeble visible connection with the visible sector, in the presence of any thermal DM.(DM2). We propose to classify this new kind of DM as pseudo-FIMP (pFIMP) which has unique characteristics impacting the relic density, direct, and collider search implications. We studied it in a model-independent manner by solving coupled Boltzmann Equations (cBEQ) and also for a toy model with two-component real scalar DM.
In this work, we have carried out the study of a traversable wormhole in the dark matter halo. We have formulated the exact solution of the spherically symmetric traversable wormhole with isotropic pressure conditions...
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In this work, we have carried out the study of a traversable wormhole in the dark matter halo. We have formulated the exact solution of the spherically symmetric traversable wormhole with isotropic pressure conditions by using the Jaffe dark matter density profile. The Jaffe profile produces a suitable shape function that meets all the requirements for presenting the wormhole geometries. We have investigated all the necessary energy conditions viz., null energy condition(NEC), weak energy condition(WEC), strong energy condition(SEC), and dominant energy conditions(DEC) for the considered wormhole. All the suitable stability conditions are analyzed and explained by related plots.
We investigate the comparative study of mass varying neutrino and canonical scalar field (quintessence) as a source of dark energy in the spatially flat (k = 0) universe. We obtained the scaling solution of dominating...
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We investigate the comparative study of mass varying neutrino and canonical scalar field (quintessence) as a source of dark energy in the spatially flat (k = 0) universe. We obtained the scaling solution of dominating components of the universe in the absence of interaction between them.
Inconsistencies between the predictions based on the Lambda CDM model and astrophysical observations at dwarf and galaxy scales motivate alternatives to WIMPs. A compelling alternative is the self-interacting dark mat...
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Inconsistencies between the predictions based on the Lambda CDM model and astrophysical observations at dwarf and galaxy scales motivate alternatives to WIMPs. A compelling alternative is the self-interacting dark matter (SIDM), which not only addresses the anomalies on small scales but also aligns seamlessly with the large-scale Lambda CDM predictions. Nevertheless, the thermal relic of SIDM tends to be under-abundant within the standard cosmological framework, which considers dark matter decoupling from the cosmic soup in a radiation-dominated epoch. To tackle this challenge, our approach involves introducing a non-standard expansion history of the universe by incorporating a non-radiation-like component into the cosmic soup. In this modified scenario, SIDM decouples at an early epoch compared to the standard model, resulting in an enhanced relic density that matches observed values. We consider our SIDM candidate to be a pseudo-Dirac fermion to nullify its diagonal vector interaction, thereby circumventing direct search constraints. Through this, we identify a parameter space that remains consistent with astrophysical observations and relic density criteria.
In this work, we investigate the existence of one zero texture and one vanishing subtrace in the Majorana neutrino mass matrix. There are a total of thirty-six possible textures of neutrino mass matrix with the constr...
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In this work, we investigate the existence of one zero texture and one vanishing subtrace in the Majorana neutrino mass matrix. There are a total of thirty-six possible textures of neutrino mass matrix with the constrained conditions of one zero texture and one vanishing subtrace. Here we explore the phenomenological implications of only two classes of textures, i.e., Class A and Class B. We analyze the viability of all the textures using the ratio of the solar and atmospheric mass-squared differences (R-nu). Out of 12 textures of both the classes, only one texture (A(1)) from class A and three textures (B-1, B-4 and B-5) from class B are found to be viable under the current neutrino oscillation data at 3 sigma confidence level. Finally, we study the ranges of the Majorana Phases (alpha and beta) for the allowed range of the Dirac CP phase, delta for all the viable textures.
In our work, we have used modular invariance approach to construct a neutrino mass model in the framework of the inverse seesaw mechanism with modular S-4 flavor symmetry which requires less number of flavon fields. T...
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In our work, we have used modular invariance approach to construct a neutrino mass model in the framework of the inverse seesaw mechanism with modular S-4 flavor symmetry which requires less number of flavon fields. The phenomenological study of the neutrino mass matrix is carried out and correlation plots are drawn using the current 3 sigma ranges of neutrino oscillation data to test the compatibility of the model with experiments. Again the use of inverse seesaw mechanism allows the right-handed neutrinos to have masses in the TeV scale which may be feasible at the current large hadron collider experiment.
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