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Related papers: Getting the most from NOvA and T2K

200 papers

We apply Koide's mass relation of charged leptons to neutrinos and quarks, with both the normal and inverted mass schemes of neutrinos discussed. We introduce the parameters $k_{\nu}$, $k_u$ and $k_d$ to describe the deviations of neutrinos…

High Energy Physics - Phenomenology · Physics 2009-11-11 Nan Li , Bo-Qiang Ma

I attempt to quantify how far from maximal one should expect the atmospheric mixing angle to be given a neutrino mass-matrix that leads, at zeroth order, to a nu_3 mass-eigenstate that is 0% nu_e, 50% nu_mu, and 50% nu_tau. This is done by…

High Energy Physics - Phenomenology · Physics 2009-11-10 Andre de Gouvea

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

Assuming the same form of all mass matrices as motivated by quark-lepton symmetry, we discuss conditions under which bi-large mixing in the lepton sector can be obtained with a minimal amount of fine tuning requirements for possible models.…

High Energy Physics - Phenomenology · Physics 2009-11-10 Radovan Dermisek

Determining the absolute masses of neutrinos is of fundamental importance in particle physics, nuclear physics, and astrophysics. We conjecture that intrinsic mass relations exist between leptons and quarks. Using these relations and…

High Energy Physics - Phenomenology · Physics 2015-06-05 Fu-Guang Cao

Recent neutrino experiments have made very significant progresses and our knowledge of neutrino masses and mixing has considerably improved. In a model independent Monte Carlo approach, we have examined a very large class of textures, in…

High Energy Physics - Phenomenology · Physics 2007-06-22 V. Antonelli , F. Caravaglios , R. Ferrari , M. Picariello

The correct quark and charged lepton mass matrices along with a nearly correct CKM matrix may be naturally accommodated in a Pati-Salam model constructed from intersecting D6 branes on a $T^6/(\Z_2 \times \Z_2)$ orientifold. Furthermore,…

High Energy Physics - Phenomenology · Physics 2020-01-01 Jordan Gemmill , Evan Howington , Van E. Mayes

A very simple extension of the standard model to include an Abelian family symmetry is able to describe the hierarchy of quark and lepton masses and their mixing angles together with the unification of gauge couplings. We consider the…

High Energy Physics - Phenomenology · Physics 2011-07-19 H. Dreiner , G. K. Leontaris , S. Lola , Graham G. Ross , C. Scheich

Angular-energy distributions are studied for charged leptons and neutrinos from the decays of polarised top quarks. A small admixture of V+A interactions is incorporated. The polarisation dependent part of the neutrino distribution which…

High Energy Physics - Phenomenology · Physics 2009-10-28 M. Jeżabek , J. H. Kühn

We propose a model-independent analysis of the neutrino mass matrix through an expansion in terms of the eigenvectors defining the lepton mixing matrix, which we show can be parametrized as small perturbations of the tribimaximal mixing…

High Energy Physics - Phenomenology · Physics 2013-06-05 D. Aristizabal Sierra , I. de Medeiros Varzielas , E. Houet

Now that theta13 is known to be large, a medium baseline reactor experiment can observe the fine structure of the electron antineutrino survival probability curve, approximately periodic oscillations in L/E with wavelength 4pi/Delta M^2_31.…

High Energy Physics - Experiment · Physics 2015-06-11 Emilio Ciuffoli , Jarah Evslin , Xinmin Zhang

In this paper we rewrite the neutrino mixing angles and mass squared differences in matter given, in our original paper, in a notation that is more conventional for the reader. Replacing the usual neutrino mixing angles and mass squared…

High Energy Physics - Phenomenology · Physics 2018-06-26 Peter B. Denton , Hisakazu Minakata , Stephen J. Parke

Even if quark and lepton masses are not uniquely predicted by the fundamental theory, as may be the case in the string theory landscape, nevertheless their pattern may reveal features of the underlying theory. We use statistical techniques…

High Energy Physics - Phenomenology · Physics 2014-11-18 John F. Donoghue , Koushik Dutta , Andreas Ross

Neutrino oscillations change when in media in comparison to vacuum oscillations due to the scattering of neutrinos on matter constituents, electrons particularly. This can be easily described by introducing new effective matter mixing…

High Energy Physics - Phenomenology · Physics 2018-10-02 Tomas Nosek

I try to give an overview of future prospects of the experimental exploration of the unknowns in the neutrino mass pattern and the lepton flavor mixing. Because of the nature of the lectures on which this manuscript is based, I give some…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hisakazu Minakata

We present a model of neutrino masses within the framework of the EW-$\nu_R$ model in which the experimentally desired form of the PMNS matrix is obtained by applying an $A_4$ symmetry to the \emph{Higgs singlet sector} responsible for the…

High Energy Physics - Phenomenology · Physics 2015-10-28 P. Q. Hung , Trinh Le

Neutrino mixing is studied from a symmetry perspective, both bottom-up and top-down. In the bottom-up approach, we start from the tri-bimaximal mixing, or one of its three partial patterns, and construct a list of horizontal symmetry groups…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. S. Lam

We derive the lower bound on absolute scale of lightest neutrino mass for normal hierarchy and inverted hierarchy pattern of light neutrinos by studying the new physics contributions to charged lepton flavour violating decays and…

High Energy Physics - Phenomenology · Physics 2022-07-25 Prativa Pritimita , Urjit A. Yajnik , Nitali Dash , Sudhanwa Patra

The T2K experiment is a long-baseline neutrino oscillation experiment. Its main goal is to measure the last unknown lepton sector mixing angle {\theta}_{13} by observing {\nu}_e appearance in a {\nu}_{\mu} beam. It also aims to make a…

Instrumentation and Detectors · Physics 2019-08-14 T2K Collaboration , K. Abe , N. Abgrall , H. Aihara , Y. Ajima , J. B. Albert , D. Allan , P. -A. Amaudruz , C. Andreopoulos , B. Andrieu , M. D. Anerella , C. Angelsen , S. Aoki , O. Araoka , J. Argyriades , A. Ariga , T. Ariga , S. Assylbekov , J. P. A. M. de André , D. Autiero , A. Badertscher , O. Ballester , M. Barbi , G. J. Barker , P. Baron , G. Barr , L. Bartoszek , M. Batkiewicz , F. Bay , S. Bentham , V. Berardi , B. E. Berger , H. Berns , I. Bertram , M. Besnier , J. Beucher , D. Beznosko , S. Bhadra , P. Birney , D. Bishop , E. Blackmore , F. d. M. Blaszczyk , J. Blocki , A. Blondel , A. Bodek , C. Bojechko , J. Bouchez , T. Boussuge , S. B. Boyd , M. Boyer , N. Braam , R. Bradford , A. Bravar , K. Briggs , J. D. Brinson , C. Bronner , D. G. Brook-Roberge , M. Bryant , N. Buchanan , H. Budd , M. Cadabeschi , R. G. Calland , D. Calvet , J. Caravaca Rodríguez , J. Carroll , S. L. Cartwright , A. Carver , R. Castillo , M. G. Catanesi , C. Cavata , A. Cazes , A. Cervera , J. P. Charrier , C. Chavez , S. Choi , S. Chollet , G. Christodoulou , P. Colas , J. Coleman , W. Coleman , G. Collazuol , K. Connolly , P. Cooke , A. Curioni , A. Dabrowska , I. Danko , R. Das , G. S. Davies , S. Davis , M. Day , X. De La Broise , P. de Perio , G. De Rosa , T. Dealtry , A. Debraine , E. Delagnes , A. Delbart , C. Densham , F. Di Lodovico , S. Di Luise , P. Dinh Tran , J. Dobson , J. Doornbos , U. Dore , O. Drapier , F. Druillole , F. Dufour , J. Dumarchez , T. Durkin , S. Dytman , M. Dziewiecki , M. Dziomba , B. Ellison , S. Emery , A. Ereditato , J. E. Escallier , L. Escudero , L. S. Esposito , W. Faszer , M. Fechner , A. Ferrero , A. Finch , C. Fisher , M. Fitton , R. Flight , D. Forbush , E. Frank , K. Fransham , Y. Fujii , Y. Fukuda , M. Gallop , V. Galymov , G. L. Ganetis , F. C. Gannaway , A. Gaudin , J. Gaweda , A. Gendotti , M. George , S. Giffin , C. Giganti , K. Gilje , I. Giomataris , J. Giraud , A. K. Ghosh , T. Golan , M. Goldhaber , J. J. Gomez-Cadenas , S. Gomi , M. Gonin , M. Goyette , A. Grant , N. Grant , F. Grañena , S. Greenwood , P. Gumplinger , P. Guzowski , M. D. Haigh , K. Hamano , C. Hansen , T. Hara , P. F. Harrison , B. Hartfiel , M. Hartz , T. Haruyama , R. Hasanen , T. Hasegawa , N. C. Hastings , S. Hastings , A. Hatzikoutelis , K. Hayashi , Y. Hayato , T. D. J. Haycock , C. Hearty , R. L. Helmer , R. Henderson , S. Herlant , N. Higashi , J. Hignight , K. Hiraide , E. Hirose , J. Holeczek , N. Honkanen , S. Horikawa , A. Hyndman , A. K. Ichikawa , K. Ieki , M. Ieva , M. Iida , M. Ikeda , J. Ilic , J. Imber , T. Ishida , C. Ishihara , T. Ishii , S. J. Ives , M. Iwasaki , K. Iyogi , A. Izmaylov , B. Jamieson , R. A. Johnson , K. K. Joo , G. Jover-Manas , C. K. Jung , H. Kaji , T. Kajita , H. Kakuno , J. Kameda , K. Kaneyuki , D. Karlen , K. Kasami , V. Kasey , I. Kato , H. Kawamuko , E. Kearns , L. Kellet , M. Khabibullin , M. Khaleeq , N. Khan , A. Khotjantsev , D. Kielczewska , T. Kikawa , J. Y. Kim , S. -B. Kim , N. Kimura , B. Kirby , J. Kisiel , P. Kitching , T. Kobayashi , G. Kogan , S. Koike , T. Komorowski , A. Konaka , L. L. Kormos , A. Korzenev , K. Koseki , Y. Koshio , Y. Kouzuma , K. Kowalik , V. Kravtsov , I. Kreslo , W. Kropp , H. Kubo , J. Kubota , Y. Kudenko , N. Kulkarni , L. Kurchaninov , Y. Kurimoto , R. Kurjata , Y. Kurosawa , T. Kutter , J. Lagoda , K. Laihem , R. Langstaff , M. Laveder , T. B. Lawson , P. T. Le , A. Le Coguie , M. Le Ross , K. P. Lee , M. Lenckowski , C. Licciardi , I. T. Lim , T. Lindner , R. P. Litchfield , A. Longhin , G. D. Lopez , P. Lu , L. Ludovici , T. Lux , M. Macaire , L. Magaletti , K. Mahn , Y. Makida , C. J. Malafis , M. Malek , S. Manly , A. Marchionni , C. Mark , A. D. Marino , A. J. Marone , J. Marteau , J. F. Martin , T. Maruyama , T. Maryon , J. Marzec , P. Masliah , E. L. Mathie , C. Matsumura , K. Matsuoka , V. Matveev , K. Mavrokoridis , E. Mazzucato , N. McCauley , K. S. McFarland , C. McGrew , T. McLachlan , I. Mercer , M. Messina , W. Metcalf , C. Metelko , M. Mezzetto , P. Mijakowski , C. A. Miller , A. Minamino , O. Mineev , S. Mine , R. E. Minvielle , G. Mituka , M. Miura , K. Mizouchi , J. -P. Mols , L. Monfregola , E. Monmarthe , F. Moreau , B. Morgan , S. Moriyama , D. Morris , A. Muir , A. Murakami , J. F. Muratore , M. Murdoch , S. Murphy , J. Myslik , G. Nagashima , T. Nakadaira , M. Nakahata , T. Nakamoto , K. Nakamura , S. Nakayama , T. Nakaya , D. Naples , B. Nelson , T. C. Nicholls , K. Nishikawa , H. Nishino , K. Nitta , F. Nizery , J. A. Nowak , M. Noy , Y. Obayashi , T. Ogitsu , H. Ohhata , T. Okamura , K. Okumura , T. Okusawa , C. Ohlmann , K. Olchanski , R. Openshaw , S. M. Oser , M. Otani , R. A. Owen , Y. Oyama , T. Ozaki , M. Y. Pac , V. Palladino , V. Paolone , P. Paul , D. Payne , G. F. Pearce , C. Pearson , J. D. Perkin , M. Pfleger , F. Pierre , D. Pierrepont , P. Plonski , P. Poffenberger , E. Poplawska , B. Popov , M. Posiadala , J. -M. Poutissou , R. Poutissou , R. Preece , P. Przewlocki , W. Qian , J. L. Raaf , E. Radicioni , K. Ramos , P. Ratoff , T. M. Raufer , M. Ravonel , M. Raymond , F. Retiere , D. Richards , J. -L. Ritou , A. Robert , P. A. Rodrigues , E. Rondio , M. Roney , M. Rooney , D. Ross , B. Rossi , S. Roth , A. Rubbia , D. Ruterbories , R. Sacco , S. Sadler , K. Sakashita , F. Sanchez , A. Sarrat , K. Sasaki , P. Schaack , J. Schmidt , K. Scholberg , J. Schwehr , M. Scott , D. I. Scully , Y. Seiya , T. Sekiguchi , H. Sekiya , G. Sheffer , M. Shibata , Y. Shimizu , M. Shiozawa , S. Short , M. Siyad , D. Smith , R. J. Smith , M. Smy , J. Sobczyk , H. Sobel , S. Sooriyakumaran , M. Sorel , J. Spitz , A. Stahl , P. Stamoulis , O. Star , J. Statter , L. Stawnyczy , J. Steinmann , J. Steffens , B. Still , M. Stodulski , J. Stone , C. Strabel , T. Strauss , R. Sulej , P. Sutcliffe , A. Suzuki , K. Suzuki , S. Suzuki , S. Y. Suzuki , Y. Suzuki , Y. Suzuki , J. Swierblewski , T. Szeglowski , M. Szeptycka , R. Tacik , M. Tada , A. S. Tadepalli , M. Taguchi , S. Takahashi , A. Takeda , Y. Takenaga , Y. Takeuchi , H. A. Tanaka , K. Tanaka , M. Tanaka , M. M. Tanaka , N. Tanimoto , K. Tashiro , I. J. Taylor , A. Terashima , D. Terhorst , R. Terri , L. F. Thompson , A. Thorley , M. Thorpe , W. Toki , T. Tomaru , Y. Totsuka , C. Touramanis , T. Tsukamoto , V. Tvaskis , M. Tzanov , Y. Uchida , K. Ueno , M. Usseglio , A. Vacheret , M. Vagins , J. F. Van Schalkwyk , J. -C. Vanel , G. Vasseur , O. Veledar , P. Vincent , T. Wachala , A. V. Waldron , C. W. Walter , P. J. Wanderer , M. A. Ward , G. P. Ward , D. Wark , D. Warner , M. O. Wascko , A. Weber , R. Wendell , J. Wendland , N. West , L. H. Whitehead , G. Wikström , R. J. Wilkes , M. J. Wilking , Z. Williamson , J. R. Wilson , R. J. Wilson , K. Wong , T. Wongjirad , S. Yamada , Y. Yamada , A. Yamamoto , K. Yamamoto , Y. Yamanoi , H. Yamaoka , C. Yanagisawa , T. Yano , S. Yen , N. Yershov , M. Yokoyama , A. Zalewska , J. Zalipska , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito , J. Zmuda

We discuss first the flavor mixing of the quarks, using the texture zero mass matrices. Then we study a similar model for the mass matrices of the leptons. We are able to relate the mass eigenvalues of the charged leptons and of the…

High Energy Physics - Phenomenology · Physics 2010-02-16 H. Fritzsch