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Models of neutrino mixing involving one or more sterile neutrinos have resurrected their importance in the light of recent cosmological data. In this case, reactor antineutrino experiments offer an ideal place to look for signatures of…

High Energy Physics - Phenomenology · Physics 2014-08-25 Ivan Girardi , Davide Meloni , Tommy Ohlsson , He Zhang , Shun Zhou

Stimulated by recent T2K indications on a surprisingly large neutrino mixing theta_13 angle we suggest that this last unknown angle is not independent but determined by the known large solar and atmospheric neutrino oscillation angles via…

General Physics · Physics 2013-02-11 E. M. Lipmanov

Nonzero and relatively large of $\theta_{13}$ mixing angle has some phenomenological consequences on neutrino physics beyond the standard model. One of the consequences if the mixing angle $\theta_{13}\neq 0$ is the possibility of the CP…

High Energy Physics - Phenomenology · Physics 2014-10-16 Asan Damanik

We diagonalize Majorana neutrino mass matrix with the help of PMNS matrix and obtain analytical relations between the mass matrix elements and mixing parameters, viz., three mixing angles- $\theta_{12}, \theta_{23}, \theta_{13}$ and Dirac…

High Energy Physics - Phenomenology · Physics 2019-05-21 Chandan Duarah

Exchange $\mu-\tau$ symmetry in the effective Majorana neutrino mass matrix does predict a maximal mixing for atmospheric neutrino oscillations asides to a null mixing that cannot be straightforwardly identified with reactor neutrino…

High Energy Physics - Phenomenology · Physics 2022-01-05 Abdel Pérez-Lorenzana

The neutrino mixing parameters are thoroughly studied using renormalization-group evolution of Dirac neutrinos with recently proposed parametrization of the neutrino mixing angles referred as `high-scale mixing relations'. The correlations…

High Energy Physics - Phenomenology · Physics 2017-04-07 Gauhar Abbas , Mehran Zahiri Abyaneh , Rahul Srivastava

The T2K experiment presents new measurements of neutrino oscillation parameters using $19.7(16.3)\times10^{20}$ protons on target (POT) in (anti-)neutrino mode at the far detector (FD). Compared to the previous analysis, an additional…

High Energy Physics - Experiment · Physics 2023-09-12 The T2K Collaboration , K. Abe , N. Akhlaq , R. Akutsu , A. Ali , S. Alonso Monsalve , C. Alt , C. Andreopoulos , M. Antonova , S. Aoki , T. Arihara , Y. Asada , Y. Ashida , E. T. Atkin , M. Barbi , G. J. Barker , G. Barr , D. Barrow , M. Batkiewicz-Kwasniak , F. Bench , V. Berardi , L. Berns , S. Bhadra , A. Blanchet , A. Blondel , S. Bolognesi , T. Bonus , S. Bordoni , S. B. Boyd , A. Bravar , C. Bronner , S. Bron , A. Bubak , M. Buizza Avanzini , J. A. Caballero , N. F. Calabria , S. Cao , D. Carabadjac , A. J. Carter , S. L. Cartwright , M. G. Catanesi , A. Cervera , J. Chakrani , D. Cherdack , P. S. Chong , G. Christodoulou , A. Chvirova , M. Cicerchia , J. Coleman , G. Collazuol , L. Cook , A. Cudd , C. Dalmazzone , T. Daret , Yu. I. Davydov , A. De Roeck , G. De Rosa , T. Dealtry , C. C. Delogu , C. Densham , A. Dergacheva , F. Di Lodovico , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , A. J. Finch , G. A. Fiorentini Aguirre , G. Fiorillo , M. D. Fitton , J. M. Franco Patiño , M. Friend , Y. Fujii , Y. Fukuda , K. Fusshoeller , L. Giannessi , C. Giganti , V. Glagolev , M. Gonin , J. González Rosa , E. A. G. Goodman , A. Gorin , M. Grassi , M. Guigue , D. R. Hadley , J. T. Haigh , P. Hamacher-Baumann , D. A. Harris , M. Hartz , T. Hasegawa , S. Hassani , N. C. Hastings , Y. Hayato , D. Henaff , A. Hiramoto , M. Hogan , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , M. Ishitsuka , H. T. Israel , K. Iwamoto , A. Izmaylov , N. Izumi , M. Jakkapu , B. Jamieson , S. J. Jenkins , C. Jesús-Valls , J. J. Jiang , P. Jonsson , S. Joshi , C. K. Jung , P. B. Jurj , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , S. P. Kasetti , Y. Kataoka , Y. Katayama , T. Katori , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kikutani , S. King , V. Kiseeva , J. Kisiel , T. Kobata , H. Kobayashi , T. Kobayashi , L. Koch , S. Kodama , A. Konaka , L. L. Kormos , Y. Koshio , A. Kostin , T. Koto , K. Kowalik , Y. Kudenko , Y. Kudo , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , M. La Commara , L. Labarga , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , M. Lamoureux , A. Langella , J. -F. Laporte , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , Y. Lee , C. Lin , S. -K. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , K. R. Long , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , M. Mandal , S. Manly , A. D. Marino , L. Marti-Magro , D. G. R. Martin , M. Martini , J. F. Martin , T. Maruyama , T. Matsubara , V. Matveev , C. Mauger , K. Mavrokoridis , E. Mazzucato , N. McCauley , J. McElwee , K. S. McFarland , C. McGrew , J. McKean , A. Mefodiev , G. D. Megias , P. Mehta , L. Mellet , C. Metelko , M. Mezzetto , E. Miller , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , L. Munteanu , K. Nagai , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , A. Nakamura , H. Nakamura , K. Nakamura , K. D. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , T. V. Ngoc , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , K. Nishizaki , T. Nosek , F. Nova , P. Novella , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , T. Ogawa , R. Okada , W. Okinaga , K. Okumura , T. Okusawa , N. Ospina , R. A. Owen , Y. Oyama , V. Palladino , V. Paolone , M. Pari , J. Parlone , S. Parsa , J. Pasternak , M. Pavin , D. Payne , G. C. Penn , D. Pershey , L. Pickering , C. Pidcott , G. Pintaudi , C. Pistillo , B. Popov , K. Porwit , M. Posiadala-Zezula , Y. S. Prabhu , F. Pupilli , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , M. A. Ramírez , P. N. Ratoff , M. Reh , C. Riccio , E. Rondio , S. Roth , N. Roy , A. Rubbia , A. C. Ruggeri , C. A. Ruggles , A. Rychter , K. Sakashita , F. Sánchez , G. Santucci , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , A. Shaikhiev , F. Shaker , A. Shaykina , M. Shiozawa , W. Shorrock , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , A. J. Speers , R. Spina , I. A. Suslov , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , S. Tairafune , S. Takayasu , A. Takeda , Y. Takeuchi , K. Takifuji , H. K. Tanaka , Y. Tanihara , M. Tani , A. Teklu , V. V. Tereshchenko , N. Teshima , N. Thamm , L. F. Thompson , W. Toki , C. Touramanis , T. Towstego , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , D. Vargas , M. Varghese , G. Vasseur , C. Vilela , E. Villa , W. G. S. Vinning , U. Virginet , T. Vladisavljevic , T. Wachala , J. G. Walsh , Y. Wang , L. Wan , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , Y. -h. Xu , K. Yamamoto , T. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , M. Yu , R. Zaki , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , X. Zhao , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

Based on Friedberg and Lee's geometric picture by which the tribimaximal Pontecorvo-Maki-Nakawaga-Sakata leptonic mixing matrix is constructed, namely, corresponding mixing angles correspond to the geometric angles among the sides of a…

High Energy Physics - Phenomenology · Physics 2013-05-29 Jun-Mou Chen , Bin Wang , Xue-Qian Li

In 2004, two of us proposed a texture, the "Simplest" neutrino mass matrix, which predicted sin(theta13)=sqrt((2 Solar-Delta m^2)/(3 Atm-Delta m^2)) and delta_CP=90 degrees. Using today's measured values for neutrino mass-squared…

High Energy Physics - Phenomenology · Physics 2013-07-31 R. Krishnan , P. F. Harrison , W. G. Scott

Leptonic CP Violating Phase $ \delta_{CP} $ in the light neutrino sector and leptogenesis via present matter antimatter asymmetry of the Universe entails each other. Probing CP violation in light neutrino oscillation is one of the…

High Energy Physics - Phenomenology · Physics 2021-03-24 Gayatri Ghosh

A recent neutrino experiment at Daya Bay gives superior data of the distribution of the prompt energy. In this paper, the energy distribution presented in the experiment is simulated by applying a Gaussian-like packet to the neutrino wave…

High Energy Physics - Phenomenology · Physics 2015-06-24 Rong-Sheng Han , Liang Chen , Ke-Lin Wang

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 discuss to what extent future precision measurements of neutrino mixing observables will influence the information we can draw from a measurement of (or an improved limit on) neutrinoless double beta decay. Whereas the Delta m^2…

High Energy Physics - Phenomenology · Physics 2009-11-11 S. Choubey , W. Rodejohann

Motivated by recent measurements which strongly support a nonzero reactor mixing angle $\theta_{13}$, we study a deviation from $S_3$ neutrino discrete symmetry by explicitly breaking the neutrino mass matrix with a general retrocirculant…

High Energy Physics - Phenomenology · Physics 2013-08-13 H. B. Benaoum

We investigate a relation among neutrino observables, three mixing angles and two mass squared differences, from a cascade texture of neutrino mass matrix. We show an allowed region of the correlation by use of current data of neutrino…

High Energy Physics - Phenomenology · Physics 2011-08-17 Naoyuki Haba , Ryo Takahashi

We propose a generalized version of the Tri-Bi-Maximal (TBM) ansatz for lepton mixing, leading to non-zero reactor angle $\theta_{13}$ and CP violation. The latter is characterized by two CP phases. The Dirac phase affecting neutrino…

High Energy Physics - Phenomenology · Physics 2018-09-19 Peng Chen , Salvador Centelles Chuliá , Gui-Jun Ding , Rahul Srivastava , José W. F. Valle

The recent measurement of the third lepton mixing angle, \theta_{13}, has shown that, although small compared to \theta_{12} and \theta_{23}, it is much larger than anticipated in schemes that generate Tri-Bi-Maximal (TBM) or Golden Ratio…

High Energy Physics - Phenomenology · Physics 2015-06-15 L. J. Hall , G. G. Ross

The long baseline neutrino experiment, T2K, and the reactor experiment, Double Chooz will soon present new data. If we expect $\sin\theta_{13}$ to be 0.1-0.2, which is close to the present experimental upper bound, we should not persist in…

High Energy Physics - Phenomenology · Physics 2011-08-30 Yusuke Shimizu , Morimitsu Tanimoto , Atsushi Watanabe

The Delta m^2_13 oscillation frequency for reactor neutrinos differs by 6.4% between normal and inverted mass hierarchy. This frequency difference accumulates to a phase difference over distance and time. The optimal distance is when the…

High Energy Physics - Phenomenology · Physics 2013-06-24 John LoSecco

T2K is a long baseline neutrino experiment which exploits a neutrino and antineutrino beam at JPARC to perform precision measurements of neutrino oscillation parameters $\Delta {\rm m}^2_{\rm 32}$, $\sin^2 \theta_{23}$ (besides the…

High Energy Physics - Experiment · Physics 2022-07-15 Ajmi Ali