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Many experiments are currently looking for evidence of neutrino mass in the form of neutrino oscillations. Oscillation probabilities are non-linear functions of the neutrino mixing matrix elements, so most comparisons of data to theory are…

High Energy Physics - Phenomenology · Physics 2007-05-23 Doris Jeanne Wagner

This review summarizes recent experimental and theoretical progress in determining neutrino mixing angles and masses through neutrino oscillations. We describe the basic physics of oscillation phenomena in vacuum and matter, as well as the…

Nuclear Theory · Physics 2015-06-15 A. B. Balantekin , W. C. Haxton

A neutrino mass model is suggested within an $SU(4)\times U(1)$ -- electroweak theory. The smallness of neutrino masses can be guaranteed by a seesaw mechanism realized through Yukawa couplings to a scalar $SU(4)$-decuplet. In this scheme…

High Energy Physics - Phenomenology · Physics 2019-10-22 N. Anh Ky , N. T. Hong Van , D. Nguyen Dinh , P. Quang Van

What information about the neutrino mass spectrum and mixing matrix can be inferred from the existing neutrino oscillation data? We discuss here the answer to this question in the case of mixing of three and four neutrinos. We present the…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. M. Bilenky , C. Giunti , W. Grimus

Certainly one of the most exciting areas of research at present is neutrino physics. The neutrinos are fantastically numerous in the universe and as such they have bearing on our understanding of the universe. Therefore, we must understand…

High Energy Physics - Phenomenology · Physics 2007-05-23 Riazuddin

We discuss some known approaches and results as well as few new ideas concerning origins and nature of neutrino mass. The key issues include (i) connections of neutrino and charged fermions masses, relation between masses and mixing, energy…

High Energy Physics - Phenomenology · Physics 2015-02-17 A. Yu. Smirnov

We have shown previously that the mass of the muon neutrino can be determined from the energy released in the decay of the pi (+-) mesons, and that the mass of the electron neutrino can be determined from the energy released in the decay of…

General Physics · Physics 2007-05-23 E. L. Koschmieder

The landmark discovery that neutrinos have mass and can change type (or "flavor") as they propagate -- a process called neutrino oscillation -- has opened up a rich array of theoretical and experimental questions being actively pursued…

High Energy Physics - Experiment · Physics 2025-10-28 NOvA , T2K Collaborations , : , K. Abe , S. Abe , S. Abubakar , M. A. Acero , B. Acharya , P. Adamson , H. Adhkary , R. Akutsu , H. Alarakia-Charles , Y. I. Alj Hakim , S. Alonso Monsalve , N. Anfimov , L. Anthony , A. Antoshkin , S. Aoki , K. A. Apte , T. Arai , T. Arihara , S. Arimoto , E. Arrieta-Diaz , Y. Ashida , L. Asquith , E. T. Atkin , A. Aurisano , D. Azevedo , N. Babu , A. Back , N. Balashov , P. Baldi , B. A. Bambah , E. F. Bannister , V. Baranov , G. J. Barker , G. Barr , A. Barros , D. Barrow , A. Bat , P. Bates , L. Bathe-Peters , M. Batkiewicz-Kwasniak , N. Baudis , K. Bays , V. Berardi , L. Berns , R. Bernstein , T. J. C. Bezerra , V. Bhatnagar , S. Bhattacharjee , B. Bhuyan , J. Bian , A. Blanchet , A. Blondel , P. M. M. Boistier , S. Bolognesi , A. C. Booth , S. Bordoni , R. Bowles , S. B. Boyd , B. Brahma , C. Bromberg , C. Bronner , A. Bubak , N. Buchanan , M. Buizza Avanzini , A. Butkevich , J. A. Caballero , F. Cadoux , N. F. Calabria , S. Calvez , S. Cao , S. Cap , D. Carabadjac , J. M. Carceller , T. J. Carroll , S. L. Cartwright , M. P. Casado , M. G. Catanesi , E. Catano-Mur , J. P. Cesar , J. Chakrani , A. Chalumeau , D. Cherdack , R. Chirco , B. C. Choudhary , A. Christensen , A. Chvirova , M. F. Cicala , T. E. Coan , J. Coleman , G. Collazuol , T. Contreras , A. Cooleybeck , F. Cormier , D. Coveyou , A. A. L. Craplet , L. Cremonesi , A. Cudd , D. D'ago , C. Dalmazzone , T. Daret , P. Dasgupta , G. S. Davies , C. Davis , Yu. I. Davydov , P. de Perio , G. De Rosa , T. Dealtry , C. Densham , A. Dergacheva , P. F. Derwent , R. Dharmapal Banerjee , F. Di Lodovico , G. Diaz Lopez , P. Ding , Z. Djurcic , K. Dobbs , S. Dolan , M. Dolce , D. Douqa , T. A. Doyle , O. Drapier , D. Dueñas Tonguino , K. E. Duffy , E. C. Dukes , J. Dumarchez , P. Dunne , A. Dye , K. Dygnarowicz , A. Eguchi , R. Ehrlich , J. Elias , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , E. Ewart , D. Fedorova , S. Fedotov , M. Feltre , L. Feng , D. Ferlewicz , P. Filip , A. J. Finch , M. D. Fitton , C. Forza , M. J. Frank , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , H. R. Gallagher , J. García-Marcos , A. C. Germer , L. Giannessi , C. Giganti , M. Girgus , A. Giri , V. Glagolev , R. A. Gomes , M. Gonin , R. González Jiménez , J. González Rosa , E. A. G. Goodman , M. C. Goodman , K. Gorshanov , P. Govindaraj , M. Grassi , R. Group , M. Guigue , F. Y. Guo , A. Habig , D. R. Hadley , F. Hakl , S. Han , D. A. Harris , R. J. Harris , J. Hartnell , T. Hasegawa , C. M. Hasnip , S. Hassani , N. C. Hastings , R. Hatcher , Y. Hayato , J. M. Hays , M. He , I. Heitkamp , K. Heller , D. Henaff , V Hewes , A. Himmel , Y. Hino , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , M. C. F. Hooft , T. Horoho , K. Hosokawa , J. Hu , A. K. Ichikawa , K. Ieki , M. Ikeda , T. Ishida , M. Ishitsuka , A. Ivanova , A. Izmaylov , N. Jachowicz , B. Jargowsky , S. J. Jenkins , C. Jesús-Valls , J. Y. Ji , M. Jia , J. J. Jiang , T. P. Jones , P. Jonsson , S. Joshi , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , I. Kakorin , H. Kakuno , A. Kalitkina , J. Kameda , D. M. Kaplan , S. Karpova , V. S. Kasturi , Y. Kataoka , T. Katori , Y. Kawamura , M. Kawaue , E. Kearns , M. Khabibullin , A. Khanam , A. Khotjantsev , T. Kikawa , S. King , B. Kirezli , V. Kiseeva , J. Kisiel , J. Kleykamp , O. Klimov , A. Klustová , L. Kneale , H. Kobayashi , L. Koch , S. Kodama , L. W. Koerner , L. Kolupaeva , M. Kolupanova , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , R. Kralik , Y. Kudenko , Y. Kudo , A. Kumar , A. Kumar Jha , R. Kurjata , V. Kurochka , C. D. Kuruppu , V. Kus , T. Kutter , L. Labarga , M. Lachat , K. Lachner , T. Lackey , J. Lagoda , S. M. Lakshmi , M. Lamers James , K. Lang , A. Langella , D. H. Langridge , J. -F. Laporte , P. Lasorak , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , D. Leon Silverio , J. Lesmeister , S. Levorato , S. V. Lewis , B. Li , W. Li , C. Lin , A. Lister , R. P. Litchfield , J. Liu , S. L. Liu , J. A. Lock , A. Longhin , A. Lopez Moreno , X. Lu , L. Ludovici , T. Lux , L. N. Machado , M. MacMahon , L. Magaletti , S. Magill , K. Mahn , K. K. Mahtani , M. Mandal , S. Manly , W. A. Mann , M. T. Manoharan , M. Manrique Plata , A. D. Marino , M. L. Marshak , D. G. R. Martin , L. Martinez , D. A. Martinez Caicedo , M. Martinez-Casales , M. Martini , T. Matsubara , R. Matsumoto , V. Matveev , C. Mauger , K. Mavrokoridis , N. McCauley , K. S. McFarland , C. McGrew , J. McKean , A. Mefodiev , G. D. Megias , B. Mehta , L. Mellet , M. D. Messier , C. Metelko , H. Meyer , M. Mezzetto , T. Miao , S. Miki , V. Mikola , E. W. Miller , W. H. Miller , A. Minamino , S. Mine , O. Mineev , J. Mirabito , S. R. Mishra , M. Miura , R. Mohanta , A. Moren , S. Moriyama , S. Moriyama , A. Morozova , P. Morrison , W. Mu , L. Mualem , Th. A. Mueller , M. Muether , K. Mulder , D. Munford , A. Muñoz , L. Munteanu , D. Myers , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , K. D. Nakamura , Y. Nakano , T. Nakaya , S. Nakayama , K. Nakayoshi , D. Naples , C. E. R. Naseby , S. Nelleri , J. K. Nelson , D. T. Nguyen , V. Q. Nguyen , R. Nichol , K. Niewczas , E. Niner , S. Nishimori , Y. Nishimura , Y. Noguchi , A. Norman , A. Norrick , T. Nosek , F. Nova , J. C. Nugent , H. Oh , R. Okazaki , H. M. O'Keeffe , W. Okinaga , K. Okumura , T. Okusawa , A. Olshevskiy , T. Olson , N. Onda , N. Ospina , L. Osu , L. O'Sullivan , Y. Oyama , M. Ozkaynak , A. Pal , J. Paley , L. Panda , V. Paolone , J. Pasternak , R. B. Patterson , G. Pawloski , D. Payne , T. Peacock , R. Petti , M. Pfaff , L. Pickering , R. K. Plunkett , B. Popov , J. C. C. Porter , A. J. Portocarrero Yrey , M. Posiadala-Zezula , Y. S. Prabhu , L. R. Prais , H. Prasad , F. Pupilli , B. Quilain , P. T. Quyen , E. Radicioni , B. Radics , A. Rafique , V. Raj , M. Rajaoalisoa , M. A. Ramirez , R. Ramsden , B. Ramson , P. N. Ratoff , B. Rebel , M. Reh , G. Reina , C. Riccio , D. W. Riley , E. Robles , E. Rondio , S. Roth , N. Roy , P. Roy , A. Rubbia , L. Russo , A. Rychter , W. Saenz , K. Sakashita , S. Samani , O. Samoylov , M. C. Sanchez , F. Sánchez , S. Sánchez Falero , E. M. Sandford , Y. Sato , T. Schefke , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , T. Sekiya , D. Seppala , D. Sgalaberna , A. Shaikhiev , P. Shanahan , P. Sharma , A. Sheshukov , M. Shiozawa , Y. Shiraishi , Shivam , A. Shmakov , W. Shorrock , S. Shukla , A. Shvartsman , I. Singh , P. Singh , V. Singh , S. Singh Chhibra , D. K. Singha , N. Skrobova , K. Skwarczynski , A. Smith , J. Smolik , M. Smy , D. Smyczek , P. Snopok , J. T. Sobczyk , H. Sobel , F. J. P. Soler , N. Solomey , A. Sousa , K. Soustruznik , A. J. Speers , R. Spina , A. Srivastava , P. Stowell , M. Strait , Y. Stroke , I. A. Suslov , L. Suter , A. Sutton , K. Sutton , A. Suzuki , S. Y. Suzuki , S. Swain , C. Sweeney , A. Sztuc , M. Tada , S. Tairafune , A. Takeda , Y. Takeuchi , N. Talukdar , H. K. Tanaka , H. Tanigawa , P. Tas , A. Teklu , V. V. Tereshchenko , T. Thakore , N. Thamm , J. Thomas , E. Tiras , M. Titus , Y. Torun , C. Touramanis , D. Tran , N. Tran , J. Trokan-Tenorio , T. Tsukamoto , M. Tzanov , Y. Uchida , J. Urheim , M. Vagins , P. Vahle , Z. Vallari , M. Varghese , I. Vasilyev , G. Vasseur , E. Villa , U. Virginet , T. Vladisavljevic , K. J. Vockerodt , T. Wachala , D. Wakabayashi , A. V. Waldron , H. T. Wallace , M. Wallbank , J. G. Walsh , L. Wan , T. K. Warburton , D. Wark , M. O. Wascko , A. Weber , C. Weber , R. Wendell , M. Wetstein , D. Whittington , D. A. Wickremasinghe , M. J. Wilking , C. Wilkinson , J. R. Wilson , J. Wolcott , K. Wood , C. Wret , S. Wu , W. Wu , W. Wu , J. Xia , Y. Xiao , B. Yaeggy , A. Yahaya , K. Yamamoto , T. Yamamoto , C. Yanagisawa , Y. Yang , A. Yankelevich , T. Yano , N. Yershov , U. Yevarouskaya , M. Yokoyama , K. Yonehara , Y. Yoshimoto , N. Yoshimura , S. Zadorozhnyy , R. Zaki , J. Zalesak , A. Zalewska , J. Zalipska , G. Zarnecki , J. Zhang , X. Y. Zhao , H. Zheng , H. Zhong , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos , R. Zwaska

The three active light neutrinos are used to explain the neutrino oscillations. The inherently bi-large mixing neutrino mass matrix and the Fritzsch type, bi-small mixing charged lepton mass matrix are assumed. By requiring the maximal…

High Energy Physics - Phenomenology · Physics 2014-11-17 Chun Liu , Jeonghyeon Song

The recent real time KARMEN anomaly for the electron neutrino counting rates (obtained from stopped muon decays) is analyzed by employing a neutrino flavor rotation model in which the muon neutrino is in a superposition of only two mass…

High Energy Physics - Phenomenology · Physics 2007-05-23 Y. N. Srivastava , S. Palit , A. Widom , E. Sassaroli

The emission of $\nu\bar\nu$ pairs off electrons in a polarized ultra-intense electromagnetic (e.g.\ laser) wave field is analyzed. We elaborate on the significance of non-linear electrodynamics effects (i.e., multi-photon processes) and…

High Energy Physics - Phenomenology · Physics 2011-03-22 A. I. Titov , B. Kampfer , H. Takabe , A. Hosaka

Assuming the seesaw mechanism for hierarchical neutrino masses, we calculate the heavy neutrino masses under the hypotheses that the mixing in the Dirac leptonic sector is similar to the quark mixing ($V_D \sim V_{CKM}$) and that $M_{\nu}…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Falcone

Neutrino physics has entered an era of precision measurements. With these precise measurements, we may be able to distinguish different models that have been constructed to explain the small neutrino masses and the large mixing among them.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mu-Chun Chen

The theoretical basics of neutrino mass and mixing are reviewed. Dirac and Majorana masses are explained, and added together to produce the see-saw picture of the lightness of neutrinos. This picture predicts that neutrinos are Majorana…

High Energy Physics - Phenomenology · Physics 2007-05-23 Boris Kayser

We consider the radiative generation of neutrino mass through the interactions of neutrinos with MeV dark matter. We construct a realistic renormalizable model with one scalar doublet and one complex singlet together with three light…

High Energy Physics - Phenomenology · Physics 2016-07-15 Abdesslam Arhrib , Céline Bœhm , Ernest Ma , Tzu-Chiang Yuan

I review the various mechanisms for obtaining nonzero neutrino masses. I focus on the possibility of adding one light singlet neutrino to the three known doublet neutrinos nu_e, nu_mu, and nu_tau to accommodate the totality of…

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

The neutrino produced in the pion decay reveals a new diffraction phenomenon due to many-body interactions in an intermediate time region when wave functions of the parent and daughters overlap. Because of diffraction, the probability to…

High Energy Physics - Phenomenology · Physics 2012-11-28 Kenzo Ishikawa , Yutaka Tobita

Explicit expressions for the differential and total rates and emissivities of neutrino pairs from the photo-neutrino process $e^\pm + \gamma \to e^\pm + \nu + \bar\nu$ in hot and dense matter are derived. Full information about the emitted…

Astrophysics · Physics 2009-11-10 Sharada Iyer Dutta , Sasa Ratkovic , Madappa Prakash

The prospects of using spectral measurements of solar neutrinos to distinguish different mechanisms of neutrino flavor mixing are analyzed. The mechanisms studied include the conventional mass mixing mechanism and an alternative mechanism…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. N. Leung , P. I. Krastev

If neutrinos have mass, we give reasons for a possible pattern of three (squared) mass eigenvalues: $m_1^2 \simeq (2.8 - 5.8) \, \mbox{(eV)}^2 $, $m_2^2 \simeq 0.01 \, \mbox{(eV)}^2 $, $m_3^2 \simeq (1.5 - 1) \times 10^{-4} \mbox{(eV)}^2 $.…

High Energy Physics - Phenomenology · Physics 2011-05-23 Saul Barshay , Patrick Heiliger