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The bimaximal (BM) neutrino mixing matrix was formulated in order to accommodate the data of the experimental results which indicate that both solar and atmospheric neutrino oscillation in vacuum are near maximal. But, after the T2K and…

High Energy Physics - Phenomenology · Physics 2015-05-05 Asan Damanik

We perform an updated global analysis of the known and unknown parameters of the standard $3\nu$ framework as of 2025. The known oscillation parameters include three mixing angles $(\theta_{12},\,\theta_{23},\,\theta_{13})$ and two squared…

High Energy Physics - Phenomenology · Physics 2025-03-12 Francesco Capozzi , William Giarè , Eligio Lisi , Antonio Marrone , Alessandro Melchiorri , Antonio Palazzo

Couplings between light scalar dark matter (DM) and neutrinos induce a perturbation to the neutrino mass matrix. If the DM oscillation period is smaller than ten minutes (or equivalently, the DM particle is heavier than $0.69\times10^{-17}$…

High Energy Physics - Phenomenology · Physics 2018-04-30 Jiajun Liao , Danny Marfatia , Kerry Whisnant

We study the possibility of generating non-zero reactor mixing angle $\theta_{13}$ by perturbing the $\mu-\tau$ symmetric neutrino mass matrix. The leading order $\mu-\tau$ symmetric neutrino mass matrix originates from type I seesaw…

High Energy Physics - Phenomenology · Physics 2015-06-22 Manikanta Borah , Debasish Borah , Mrinal Kumar Das , Sudhanwa Patra

The presence of approximate electron number conservation and \mu-\tau permutation symmetry of S_2 is shown to naturally provide bilarge neutrino mixing. First, the bimaximal neutrino mixing together with U_{e3}=0 is guaranteed to appear…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ichiro Aizawa , Motoyasu Ishiguro , Teruyuki Kitabayashi , Masaki Yasue

I argue that the observed flavor structures of leptons and quarks might imply the existence of certain flavor symmetries. The latter should be a good starting point to build realistic models towards deeper understanding of the fermion mass…

High Energy Physics - Phenomenology · Physics 2008-11-26 Zhi-zhong Xing

We present new $\nu_\mu\rightarrow\nu_e$, $\nu_\mu\rightarrow\nu_\mu$, $\overline{\nu}_\mu\rightarrow\overline{\nu}_e$, and $\overline{\nu}_\mu\rightarrow\overline{\nu}_\mu$ oscillation measurements by the NOvA experiment, with a 50%…

High Energy Physics - Experiment · Physics 2023-02-17 M. A. Acero , P. Adamson , L. Aliaga , N. Anfimov , A. Antoshkin , E. Arrieta-Diaz , L. Asquith , A. Aurisano , A. Back , C. Backhouse , M. Baird , N. Balashov , P. Baldi , B. A. Bambah , S. Bashar , K. Bays , R. Bernstein , V. Bhatnagar , D. Bhattarai , B. Bhuyan , J. Bian , J. Blair , A. C. Booth , R. Bowles , C. Bromberg , N. Buchanan , A. Butkevich , S. Calvez , T. J. Carroll , E. Catano-Mur , B. C. Choudhary , A. Christensen , T. E. Coan , M. Colo , L. Cremonesi , G. S. Davies , P. F. Derwent , P. Ding , Z. Djurcic , M. Dolce , D. Doyle , D. Dueñas Tonguino , E. C. Dukes , H. Duyang , R. Ehrlich , M. Elkins , E. Ewart , G. J. Feldman , P. Filip , J. Franc , M. J. Frank , H. R. Gallagher , R. Gandrajula , F. Gao , A. Giri , R. A. Gomes , M. C. Goodman , V. Grichine , M. Groh , R. Group , B. Guo , A. Habig , F. Hakl , A. Hall , J. Hartnell , R. Hatcher , H. Hausner , M. He , K. Heller , V. Hewes , A. Himmel , A. Holin , J. Huang , B. Jargowsky , J. Jarosz , F. Jediny , C. Johnson , M. Judah , I. Kakorin , D. M. Kaplan , A. Kalitkina , R. Keloth , O. Klimov , L. W. Koerner , L. Kolupaeva , S. Kotelnikov , R. Kralik , Ch. Kullenberg , M. Kubu , A. Kumar , C. D. Kuruppu , V. Kus , T. Lackey , K. Lang , P. Lasorak , J. Lesmeister , S. Lin , A. Lister , J. Liu , M. Lokajicek , S. Magill , M. Manrique Plata , W. A. Mann , M. L. Marshak , M. Martinez-Casales , V. Matveev , B. Mayes , D. P. Méndez , M. D. Messier , H. Meyer , T. Miao , W. H. Miller , S. R. Mishra , A. Mislivec , R. Mohanta , A. Moren , A. Morozova , W. Mu , L. Mualem , M. Muether , S. Mufson , K. Mulder , D. Naples , N. Nayak , J. K. Nelson , R. Nichol , E. Niner , A. Norman , A. Norrick , T. Nosek , H. Oh , A. Olshevskiy , T. Olson , J. Ott , J. Paley , R. B. Patterson , G. Pawloski , O. Petrova , R. Petti , D. D. Phan , R. K. Plunkett , J. C. C. Porter , A. Rafique , F. Psihas , V. Raj , M. Rajaoalisoa , B. Ramson , B. Rebel , P. Rojas , P. Roy , V. Ryabov , O. Samoylov , M. C. Sanchez , S. Sánchez Falero , P. Shanahan , A. Sheshukov , P. Singh , V. Singh , E. Smith , J. Smolik , P. Snopok , N. Solomey , A. Sousa , K. Soustruznik , M. Strait , L. Suter , A. Sutton , S. Swain , C. Sweeney , A. Sztuc , R. L. Talaga , B. Tapia Oregui , P. Tas , T. Thakore , R. B. Thayyullathil , J. Thomas , E. Tiras , J. Tripathi , J. Trokan-Tenorio , A. Tsaris , Y. Torun , J. Urheim , P. Vahle , Z. Vallari , J. Vasel , P. Vokac , T. Vrba , M. Wallbank , T. K. Warburton , M. Wetstein , D. Whittington , D. A. Wickremasinghe , S. G. Wojcicki , J. Wolcott , W. Wu , Y. Xiao , A. Yallappa Dombara , A. Yankelevich , K. Yonehara , S. Yu , Y. Yu , S. Zadorozhnyy , J. Zalesak , Y. Zhang , R. Zwaska

We analyse the radiative stability of the next-to-tribimaximal mixings ($NTBM$) with the variation of SUSY breaking scale ($m_S$) in MSSM, for both normal ordering (NO) and inverted ordering (IO) at the fixed input value of seesaw scale…

High Energy Physics - Phenomenology · Physics 2023-11-03 Kh. Helensana Devi , K. Sashikanta Singh , N. Nimai Singh

We propose that leptonic CP violation arises from a breaking of the mu-tau exchange symmetry in the neutrino mass matrix which in turn is indicated by the near maximal atmospheric neutrino mixing and the near zero \theta_{13}. We find that…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. N. Mohapatra , W. Rodejohann

Symmetry-based ideas, such as the quark-lepton complementarity (QLC) principle and the tri-bimaximal mixing (TBM) scheme, have been proposed to explain the observed mixing pattern of neutrinos. We argue that such symmetry relations need to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Amol Dighe , Srubabati Goswami , Probir Roy

Using the seesaw mechanism and a discrete symmetry, we construct a class of models for the neutrino mass matrix where the inverse of that matrix is the sum of a mu-tau antisymmetric background and a perturbation. We consider various…

High Energy Physics - Phenomenology · Physics 2009-11-11 Walter Grimus , Satoru Kaneko , Luis Lavoura , Hideyuki Sawanaka , Morimitsu Tanimoto

The cosmological model in which 20% of the dark matter is shared by two nearly equal mass neutrinos fits the structure of the universe on all scales. This has been motivated a $\nu_\mu$-$\nu_{\tau}$ oscillation explanation of the deficit of…

High Energy Physics - Phenomenology · Physics 2016-09-01 D. O. Caldwell , R. N. Mohapatra

In the first part of the present work the $\mu-\tau $ symmetry of the neutrino mass matrix is perturbed at its minimal level in order to produce deviation from Tri-bimaximal mixing (TBM), which includes nonzero value of reactor angle…

High Energy Physics - Phenomenology · Physics 2012-07-02 Subhankar Roy , N. Nimai Singh

The smallness of the $\theta_{13}$ mixing angle as observed in neutrino oscillation experiments can be understood through an approximated $\mu - \tau$ exchange symmetry in the neutrino mass matrix. Using recent oscillation neutrino data,…

High Energy Physics - Phenomenology · Physics 2015-10-21 Diana C. Rivera-Agudelo , Abdel Pérez-Lorenzana

Current neutrino oscillation data indicate that the $3\times 3$ Pontecorvo-Maki-Nakagawa-Sakata matrix $U$ exhibits a $\mu$-$\tau$ flavor interchange symmetry $|U^{}_{\mu i}| = |U^{}_{\tau i}|$ (for $i = 1, 2, 3$) as a good approximation.…

High Energy Physics - Phenomenology · Physics 2022-11-04 Zhi-zhong Xing

In the canonical seesaw framework flavor mixing and CP violation in weak charged-current interactions of light and heavy Majorana neutrinos are correlated with each other and described respectively by the $3\times 3$ matrices $U$ and $R$.…

High Energy Physics - Phenomenology · Physics 2022-06-22 Zhi-zhong Xing

Phenomena of neutrino oscillations are discussed on the basis of two-loop radiative neutrino mechanism. Neutrino mixings are experimentally suggested to be maximal in both atmospheric and solar neutrino oscillations. By using $L_e - L_\mu -…

High Energy Physics - Phenomenology · Physics 2007-05-23 Teruyuki Kitabayashi , Masaki Yasue

Within the type-I seesaw and in the basis where charged lepton and heavy neutrino mass matrices are real and diagonal, $\mu\tau$ symmetric four and three zero neutrino Yukawa textures are perturbed by lowest order $\mu\tau$ symmetry…

High Energy Physics - Phenomenology · Physics 2013-09-17 Biswajit Adhikary , Ambar Ghosal , Probir Roy

Neutrino oscillation data strongly support mu-tau symmetry as a good approximate flavor symmetry of the neutrino sector, which has to appear in any viable theory for neutrino mass-generation. The mu-tau breaking is not only small, but also…

High Energy Physics - Phenomenology · Physics 2015-03-13 Shao-Feng Ge , Hong-Jian He , Fu-Rong Yin

We make a theoretical attempt to compare the predictions from normal and inverted hierarchical models, within the framework of $\mu-\tau$ symmetry. We consider three major theoretical issues in a self consistent ways, viz., predictions on…

High Energy Physics - Phenomenology · Physics 2008-07-15 N. Nimai Singh , H. Zeen Devi , Mahadev Patgiri