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Related papers: $\Delta(27)$ framework for cobimaximal neutrino mi…

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The observed neutrino mixing, having a near maximal atmospheric neutrino mixing angle and a large solar mixing angle, is close to tri-bi-maximal. We argue that this structure suggests a family symmetric origin in which the magnitude of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 I. de Medeiros Varzielas , S. F. King , G. G. Ross

We propose a discrete non-abelian symmetry group which enforces maximal atmospheric neutrino mixing, while $\theta_{13} = 0$ and the solar mixing angle $\theta_{12}$ remains undetermined; without finetuning, $\theta_{12}$ will be large but…

High Energy Physics - Phenomenology · Physics 2015-06-25 W. Grimus , L. Lavoura

Hybrid leptogenesis framework combining type I and type II seesaw mechanism for neutrino mass necessarily include scattering topologies involving both the scalar triplet and the right handed neutrino. We demonstrate that a systematic…

High Energy Physics - Phenomenology · Physics 2024-06-26 Rohan Pramanick , Tirtha Sankar Ray , Arunansu Sil

Assuming Majorana nature of neutrinos, a general expression for the charged lepton corrections to scaling neutrino mixing has been obtained in the context of three flavor neutrino oscillations. Non-zero value of the reactor mixing angle is…

High Energy Physics - Phenomenology · Physics 2014-01-21 S. Dev , Radha Raman Gautam , Lal Singh

$\mu$-$\tau$ symmetry imposed on the neutrino mass matrix in the flavour basis is known to be quite predictive. We integrate this very specific neutrino symmetry into a more general framework based on the supersymmetric SO(10) grand unified…

High Energy Physics - Phenomenology · Physics 2010-11-30 Anjan S. Joshipura , Bhavik P. Kodrani , Ketan M. Patel

We analyse a flavour model for a lepton sector which is based on type I seesaw mechanism, a Z_2 symmetry for lepton flavours, a mu-tau interchange symmetry and a CP symmetry. This model fits well the data of neutrino mass squared…

High Energy Physics - Phenomenology · Physics 2015-10-19 Darius Jurciukonis , Thomas Gajdosik , Andrius Juodagalvis

We study the possibility of generating tiny neutrino mass through a combination of type I and type II seesaw mechanism within the framework of an abelian extension of standard model. The model also provides a naturally stable dark matter…

High Energy Physics - Phenomenology · Physics 2014-11-11 Arnab Dasgupta , Debasish Borah

We propose a model which uses the seesaw mechanism and the lepton number $\bar L = L_e - L_\mu - L_\tau$ to achieve the neutrino mass spectrum $m_1 = m_2$ and $m_3 = 0$, together with a lepton mixing matrix $U$ with $U_{e3} = 0$. In this…

High Energy Physics - Phenomenology · Physics 2009-10-31 W. Grimus , L. Lavoura

In the context of a typical model for fermion mass matrices, possibly based on the horizontal U(2) symmetry, we explore the effect of the type II seesaw mechanism on lepton mixings. We find that the combined contribution of type I and type…

High Energy Physics - Phenomenology · Physics 2014-11-18 D. Falcone

With the motivation of simultaneously explaining dark matter and neutrino masses, mixing angles, we have invoked the Type-II seesaw model extended by an extra $SU(2)$ doublet $\Phi$. Moreover, we have imposed a $\mathbb{Z}_2$ parity on…

High Energy Physics - Phenomenology · Physics 2019-06-07 Anirban Biswas , Avirup Shaw

We discuss the special class of models where nearly maximal neutrino mixing is produced through the see-saw mechanism, starting from only nearly diagonal matrices for charged leptons, Dirac neutrinos and Majorana right-handed neutrinos.

High Energy Physics - Phenomenology · Physics 2009-10-31 Guido Altarelli , Ferruccio Feruglio , Isabella Masina

Three of the viable solutions of the solar neutrino problem are consistent with close to maximal leptonic mixing: $\sin^2\theta_{12}={1\over2}(1-\epsilon_{12})$ with $|\epsilon_{12}|\ll1$. Flavor models can naturally explain close to…

High Energy Physics - Phenomenology · Physics 2014-11-17 Yosef Nir

Opening up the Weinberg operator at 1-loop level using a scalar triplet, two scalar doublets and one fermion gives rise to T4-2-i one-loop topology. Neutrino masses generated from this topology are always accompanied by the tree level Type…

High Energy Physics - Phenomenology · Physics 2020-12-02 M. A. Loualidi , M. Miskaoui

We propose a seesaw scenario that possible corrections to the tribimaximal pattern of lepton mixing are due to the small phase splitting of the right-handed neutrino mass matrix. we show that the small deviations can be expressed…

High Energy Physics - Phenomenology · Physics 2010-05-07 Y. F. Li , Q. Y. Liu

We investigate the possibility of expressing the charged leptons and neutrino mass matrices as linear combinations of generators of a single finite group. Constraints imposed on the resulting mixing matrix by current data restrict the group…

High Energy Physics - Phenomenology · Physics 2015-06-17 G. K. Leontaris , N. D. Vlachos

We propose a model where neutrino masses are generated at three loop order but neutrinoless double beta decay occurs at one loop. Thus we can have large neutrinoless double beta decay observable in the future experiments even when the…

High Energy Physics - Phenomenology · Physics 2018-06-21 Julien Alcaide , Dipankar Das , Arcadi Santamaria

Using the Weinberg operator, we present a full collection of genuine two-loop models for neutrino mass generation, which contain a dark matter particle as one of the internal messengers. These models can be constructed simply by adding new…

High Energy Physics - Phenomenology · Physics 2017-05-24 C. Simoes , D. Wegman

Recent (first or/and the best) results from the neutrino experiments are reviewed and their implications for the theory are discussed. The sense of the experiments is the searching for neutrino masses, mixing and interactions beyond the…

High Energy Physics - Phenomenology · Physics 2009-09-25 Alexei Yu. Smirnov

We propose a minimal model where a dark sector, odd under a $\mathcal{Z}_2$ discrete symmetry, is the seed of lepton number violation in the neutrino sector at the loop level, in the context of the linear seesaw mechanism. Neutrino mass…

High Energy Physics - Phenomenology · Physics 2023-07-19 A. Batra , H. B. Câmara , F. R. Joaquim

Discrete symmetries being preferred to explain the neutrino phenomenology, we chose the simplest $S_3$ group and explore the implication of its modular form on neutrino masses and mixing. Non-trivial transformations of Yukawa couplings…

High Energy Physics - Phenomenology · Physics 2020-08-06 Subhasmita Mishra
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