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Related papers: Hints of theta_13>0 from global neutrino data anal…

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The residual Z^s_2(k) and bar Z^s_2(k) symmetries induce a direct and unique phenomenological relation with theta_x (= theta_13) expressed in terms of the other two mixing angles, theta_s (= theta_12) and theta_a (= theta_23), and the Dirac…

High Energy Physics - Phenomenology · Physics 2013-05-30 Shao-Feng Ge , Duane A. Dicus , Wayne W. Repko

We update the analysis of the viability of the lepton mixing patterns originating from $A_4$, $S_4$ and $A_5$ discrete flavour symmetries and leading to predictions for the solar neutrino mixing angle, $\theta_{12}$. We perform a…

High Energy Physics - Phenomenology · Physics 2026-03-19 S. T. Petcov , A. V. Titov

We present the results of a global analysis of the neutrino oscillation data available as of fall 2018 in the framework of three massive mixed neutrinos with the goal at determining the ranges of allowed values for the six relevant…

High Energy Physics - Phenomenology · Physics 2019-02-19 Ivan Esteban , M. C. Gonzalez-Garcia , Alvaro Hernandez-Cabezudo , Michele Maltoni , Thomas Schwetz

The overall characteristics of the solar and atmospheric neutrino oscillation are approximately consistent with a tribimaximal form of the mixing matrix $U$ of the lepton sector. Exact tribimaximal mixing leads to $\theta_{13}=0$. However,…

High Energy Physics - Phenomenology · Physics 2016-05-03 N. Razzaghi , S. S. Gousheh

The simplest neutrino mass models based on $A_4$ symmetry predict $\theta_{13} = 0$ at tree level, a value that contradicts recent data. We study models that arise from the spontaneous breaking of an $SO(3)$ symmetry to its $A_4$ subgroup,…

High Energy Physics - Phenomenology · Physics 2015-04-16 Yuval Grossman , Wee Hao Ng

The recent discovery by the Daya-Bay and RENO experiments, that \theta_{13} is nonzero and relatively large, significantly impacts existing experiments and the planning of future facilities. In many scenarios, the nonzero value of…

High Energy Physics - Phenomenology · Physics 2012-09-05 Vernon Barger , Raj Gandhi , Pomita Ghoshal , Srubabati Goswami , Danny Marfatia , Suprabh Prakash , Sushant K. Raut , S. Uma Sankar

We study the impact of very light sterile neutrinos (Delta m^2_new around 1 to 10 times 10^(-2) eV^2, sin^2 2theta_new<10^(-1)) on upcoming theta_13-driven reactor antineutrino experiments like Double-CHOOZ and Daya Bay. Oscillations driven…

High Energy Physics - Phenomenology · Physics 2013-05-29 Andre de Gouvea , Thomas Wytock

We speculate that the mass spectrum of three neutrinos might have a normal hierarchy as that of three charged leptons or that of three up-type (or down-type) quarks. In this spirit, we propose a novel parametrization of the $3\times 3$…

High Energy Physics - Phenomenology · Physics 2009-11-11 Harald Fritzsch , Zhi-zhong Xing

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

In the original 2004 paper which first derived tribimaximal mixing in the context of A(4), i.e. the non-Abelian finite symmetry group of the tetrahedron (Plato's fire), as its simplest application, it was also pointed out how theta(13)…

High Energy Physics - Phenomenology · Physics 2011-12-26 Ernest Ma , Daniel Wegman

If the solution to the solar neutrino puzzle falls in the LMA region, KamLAND should be able to measure with good precision the corresponding oscillation parameters after a few years of data taking. Assuming a positive signal, we study…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. C. Gonzalez-Garcia , C. Peña-Garay

An approximate Z_3 family symmetry is proposed for leptons which results in a neutrino mass matrix with sin^2 2 theta_atm = 1 and tan^2 theta_sol = 0.5, but the latter value could easily be smaller. A generic requirement of this approach is…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ernest Ma

The standard three-neutrino (3nu) oscillation framework is being increasingly refined by results coming from different sets of experiments, using neutrinos from solar, atmospheric, accelerator and reactor sources. At present, each of the…

High Energy Physics - Phenomenology · Physics 2014-05-28 F. Capozzi , G. L. Fogli , E. Lisi , A. Marrone , D. Montanino , A. Palazzo

We perform global analysis of the solar neutrino data including the day and night spectra of events at SNO. In the context of two active neutrino mixing, the best fit of the data is provided by the LMA MSW solution with Delta m^2 = 6.15…

High Energy Physics - Phenomenology · Physics 2009-11-07 P. C. de Holanda , A. Yu. Smirnov

Neutrino oscillation data indicate that $\theta_{23}$ is close to $\pi/4$ and $\theta_{13}$ is very small. A simple $\mu\leftrightarrow\tau$ exchange symmetry of the neutrino mass matrix predicts $\theta_{23}=-\pi/4$ and $\theta_{13}=0$.…

High Energy Physics - Phenomenology · Physics 2018-03-13 Rambabu Korrapati , S. Uma Sankar

We use a model, with no CP violation, of the world's neutrino oscillation data, excluding the LSND experiments, and search the full parameter space ($0\leq\theta_{12} \le \pi/2$; $-\pi/2 \le \theta_{13} \le \pi/2$; and 0\leq\theta_{23} \le…

Nuclear Theory · Physics 2007-05-23 D. C. Latimer , D. J. Ernst

This Letter reports new results on muon neutrino disappearance from NOvA, using a 14 kton detector equivalent exposure of $6.05\times10^{20}$ protons-on-target from the NuMI beam at the Fermi National Accelerator Laboratory. The measurement…

High Energy Physics - Experiment · Physics 2017-04-18 The NOvA Collaboration , P. Adamson , L. Aliaga , D. Ambrose , N. Anfimov , A. Antoshkin , E. Arrieta-Diaz , K. Augsten , A. Aurisano , C. Backhouse , M. Baird , B. A. Bambah , K. Bays , B. Behera , S. Bending , R. Bernstein , V. Bhatnagar , B. Bhuyan , J. Bian , T. Blackburn , A. Bolshakova , C. Bromberg , J. Brown , G. Brunetti , N. Buchanan , A. Butkevich , V. Bychkov , M. Campbell , E. Catano-Mur , S. Childress , B. C. Choudhary , B. Chowdhury , T. E. Coan , J. A. B. Coelho , M. Colo , J. Cooper , L. Corwin , L. Cremonesi , D. Cronin-Hennessy , G. S. Davies , J. P. Davies , P. F. Derwent , S. Desai , R. Dharmapalan , P. Ding , Z. Djurcic , E. C. Dukes , H. Duyang , S. Edayath , R. Ehrlich , G. J. Feldman , M. Gabrielyan , H. R. Gallagher , S. Germani , T. Ghosh , A. Giri , R. A. Gomes , M. C. Goodman , V. Grichine , R. Group , D. Grover , B. Guo , A. Habig , J. Hartnell , R. Hatcher , A. Hatzikoutelis , K. Heller , A. Himmel , A. Holin , J. Hylen , F. Jediny , M. Judah , G. K. Kafka , D. Kalra , S. M. S. Kasahara , S. Kasetti , R. Keloth , L. Kolupaeva , S. Kotelnikov , I. Kourbanis , A. Kreymer , A. Kumar , S. Kurbanov , K. Lang , W. M. Lee , S. Lin , J. Liu , M. Lokajicek , J. Lozier , S. Luchuk , K. Maan , S. Magill , W. A. Mann , M. L. Marshak , K. Matera , V. Matveev , D. P. Méndez , M. D. Messier , H. Meyer , T. Miao , W. H. Miller , S. R. Mishra , R. Mohanta , A. Moren , L. Mualem , M. Muether , S. Mufson , R. Murphy , J. Musser , J. K. Nelson , R. Nichol , E. Niner , A. Norman , T. Nosek , Y. Oksuzian , A. Olshevskiy , T. Olson , J. Paley , P. Pandey , R. B. Patterson , G. Pawloski , D. Pershey , O. Petrova , R. Petti , S. Phan-Budd , R. K. Plunkett , R. Poling , B. Potukuchi , C. Principato , F. Psihas , A. Radovic , R. A. Rameika , B. Rebel , B. Reed , D. Rocco , P. Rojas , V. Ryabov , K. Sachdev , P. Sail , O. Samoylov , M. C. Sanchez , R. Schroeter , J. Sepulveda-Quiroz , P. Shanahan , A. Sheshukov , J. Singh , J. Singh , P. Singh , V. Singh , J. Smolik , N. Solomey , E. Song , A. Sousa , K. Soustruznik , M. Strait , L. Suter , R. L. Talaga , M. C. Tamsett , P. Tas , R. B. Thayyullathil , J. Thomas , X. Tian , S. C. Tognini , J. Tripathi , A. Tsaris , J. Urheim , P. Vahle , J. Vasel , L. Vinton , A. Vold , T. Vrba , B. Wang , M. Wetstein , D. Whittington , S. G. Wojcicki , J. Wolcott , N. Yadav , S. Yang , J. Zalesak , B. Zamorano , R. Zwaska

In the present work we propose to study neutrino oscillations employing sources of monoenergetic neutrinos following electron capture by the nucleus. Since the neutrino energy is very low the smaller of the two oscillation lengths, L23,…

High Energy Physics - Phenomenology · Physics 2014-11-21 J. D. Vergados , Yu. N. Novikov

The Double Chooz experiment has determined the value of the neutrino oscillation parameter $\theta_{13}$ from an analysis of inverse beta decay interactions with neutron capture on hydrogen. This analysis uses a three times larger fiducial…

High Energy Physics - Experiment · Physics 2013-08-30 Double Chooz Collaboration , Y. Abe , C. Aberle , J. C. dos Anjos , J. C. Barriere , M. Bergevin , A. Bernstein , T. J. C. Bezerra , L. Bezrukhov , E. Blucher , N. S. Bowden , C. Buck , J. Busenitz , A. Cabrera , E. Caden , L. Camilleri , R. Carr , M. Cerrada , P. -J. Chang , P. Chimenti , T. Classen , A. P. Collin , E. Conover , J. M. Conrad , J. I. Crespo-Anadón , K. Crum , A. Cucoanes , E. Damon , J. V. Dawson , S. Dazeley , D. Dietrich , Z. Djurcic , M. Dracos , V. Durand , J. Ebert , Y. Efremenko , M. Elnimr , A. Erickson , A. Etenko , M. Fallot , M. Fechner , F. von Feilitzsch , J. Felde , S. M. Fernandes , V. Fischer , D. Franco , A. J. Franke , M. Franke , H. Furuta , R. Gama , I. Gil-Botella , L. Giot , M. Göger-Neff , L. F. G. Gonzalez , L. Goodenough , M. C. Goodman , J. TM. Goon , D. Greiner , N. Haag , S. Habib , C. Hagner , T. Hara , F. X. Hartmann , J. Haser , A. Hatzikoutelis , T. Hayakawa , M. Hofmann , G. A. Horton-Smith , A. Hourlier , M. Ishitsuka , J. Jochum , C. Jollet , C. L. Jones , F. Kaether , L. N. Kalousis , Y. Kamyshkov , D. M. Kaplan , T. Kawasaki , G. Keefer , E. Kemp , H. de Kerret , T. Konno , D. Kryn , M. Kuze , T. Lachenmaier , C. E. Lane , C. Langbrandtner , T. Lasserre , A. Letourneau , D. Lhuillier , H. P. Lima , M. Lindner , J. M. López-Castaño , J. M. LoSecco , B. K. Lubsandorzhiev , S. Lucht , D. McKee , J. Maeda , C. N. Maesano , C. Mariani , J. Maricic , J. Martino , T. Matsubara , G. Mention , A. Meregaglia , M. Meyer , T. Miletic , R. Milincic , H. Miyata , Th. A. Mueller , Y. Nagasaka , K. Nakajima , P. Novella , M. Obolensky , L. Oberauer , A. Onillon , A. Osborn , I. Ostrovskiy , C. Palomares , I. M. Pepe , S. Perasso , P. Perrin , P. Pfahler , A. Porta , W. Potzel , G. Pronost , J. Reichenbacher , B. Reinhold , A. Remoto , M. Röhling , R. Roncin , S. Roth , B. Rybolt , Y. Sakamoto , R. Santorelli , F. Sato , S. Schönert , S. Schoppmann , T. Schwetz , M. H. Shaevitz , S. Shimojima , D. Shrestha , J-L. Sida , V. Sinev , M. Skorokhvatov , E. Smith , J. Spitz , A. Stahl , I. Stancu , L. F. F. Stokes , M. Strait , A. Stüken , F. Suekane , S. Sukhotin , T. Sumiyoshi , Y. Sun , R. Svoboda , K. Terao , A. Tonazzo , M. Toups , H. H. Trinh Thi , G. Valdiviesso , C. Veyssiere , S. Wagner , H. Watanabe , B. White , C. Wiebusch , L. Winslow , M. Worcester , M. Wurm , F. Yermia , V. Zimmer

The discovery of neutrino mixing and oscillations over the past decade provides firm evidence for new physics beyond the Standard Model. Recently, theta13 has been determined to be moderately large, quite close to its previous upper bound.…

High Energy Physics - Phenomenology · Physics 2014-01-21 Sanjib Kumar Agarwalla