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Related papers: The Last Neutrino Mixing angle theta13

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An elegant model is proposed by extending the Standard Model using the $\Delta(27)\times Z_3 \times Z_{10}$ symmetry within the framework of the Type-I + Type-II seesaw mechanism. This model is particularly noteworthy for its ability to…

High Energy Physics - Phenomenology · Physics 2025-03-26 Manash Dey , Subhankar Roy

We study in detail the sensitivity of neutrino oscillation probabilities to the fundamental neutrino parameters and their possible determination through experiments. The first part of the paper is devoted to the broad theme of isolating…

High Energy Physics - Phenomenology · Physics 2009-11-11 D. Indumathi , M. V. N. Murthy , G. Rajasekaran , Nita Sinha

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

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

Several experimental results could be interpreted as evidence that certain neutrino mixing angles are large, of order unity. However, in the context of grand unified models the neutrino angles come out characteristically to be small, like…

High Energy Physics - Phenomenology · Physics 2011-05-12 S. M. Barr

Starting with the hypothesis that quark and lepton mixings are identical at or near the GUT scale, we show that the large solar and atmospheric neutrino mixing angles together with the small reactor angle $U_{e3}$ can be understood purely…

High Energy Physics - Phenomenology · Physics 2009-11-10 R. N. Mohapatra , M. K. Parida , G. Rajasekaran

The Double-Chooz experiment goal is to search for a non-vanishing value of the Theta13 neutrino mixing angle. This is the last step to accomplish prior moving towards a new era of precision measurements in the lepton sector. The current…

High Energy Physics - Experiment · Physics 2009-11-10 Th. Lasserre

We analyze the neutrino conversions inside a supernova in the 3$\nu$ mixing scheme, and their effects on the neutrino spectra observed at the earth. We find that the observations of the energy spectra of neutrinos from a future galactic…

High Energy Physics - Phenomenology · Physics 2009-10-31 Amol S. Dighe

The near maximal value for the atmospheric neutrino mixing angle together with the fact that the solar mixing angle satisfies the relation $\sin^2\theta_\odot\simeq {1/3}$ is the basis for the so called tri-bimaximal mixing (tbm) when…

High Energy Physics - Phenomenology · Physics 2010-04-06 R. N. Mohapatra , S. Nasri , Hai-Bo Yu

We propose a flexible and model independent parametrization of the neutrino mixing matrix, which takes advantage of the fact that there are up to three small quantities in neutrino mixing phenomenology: (i) the deviation from maximal mixing…

High Energy Physics - Phenomenology · Physics 2008-11-26 W. Rodejohann

We have made improved measurements of three-flavor neutrino mixing with 19.7(16.3)$\times 10^{20}$ protons on target in (anti-)neutrino-enhanced beam modes. A new sample of muon-neutrino events with tagged pions has been added at the far…

High Energy Physics - Experiment · Physics 2026-01-01 The T2K Collaboration , K. Abe , S. Abe , R. Akutsu , H. Alarakia-Charles , Y. I. Alj Hakim , S. Alonso Monsalve , L. Anthony , S. Aoki , K. A. Apte , T. Arai , T. Arihara , S. Arimoto , Y. Ashida , E. T. Atkin , N. Babu , V. Baranov , G. J. Barker , G. Barr , D. Barrow , P. Bates , L. Bathe-Peters , M. Batkiewicz-Kwasniak , N. Baudis , V. Berardi , L. Berns , S. Bhattacharjee , A. Blanchet , A. Blondel , P. M. M. Boistier , S. Bolognesi , S. Bordoni , S. B. Boyd , C. Bronner , A. Bubak , M. Buizza Avanzini , J. A. Caballero , F. Cadoux , N. F. Calabria , S. Cao , S. Cap , D. Carabadjac , S. L. Cartwright , M. P. Casado , M. G. Catanesi , J. Chakrani , A. Chalumeau , D. Cherdack , A. Chvirova , J. Coleman , G. Collazuol , F. Cormier , A. A. L. Craplet , A. Cudd , D. D'Ago , C. Dalmazzone , T. Daret , P. Dasgupta , C. Davis , Yu. I. Davydov , P. de Perio , G. De Rosa , T. Dealtry , C. Densham , A. Dergacheva , R. Dharmapal Banerjee , F. Di Lodovico , G. Diaz Lopez , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , K. E. Duffy , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , J. Elias , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , L. Feng , D. Ferlewicz , A. J. Finch , M. D. Fitton , C. Forza , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , J. García-Marcos , A. C. Germer , L. Giannessi , C. Giganti , M. Girgus , V. Glagolev , M. Gonin , R. Gonzalez Jimenez , J. González Rosa , E. A. G. Goodman , K. Gorshanov , P. Govindaraj , M. Grassi , M. Guigue , F. Y. Guo , D. R. Hadley , S. Han , D. A. Harris , R. J. Harris , T. Hasegawa , C. M. Hasnip , S. Hassani , N. C. Hastings , Y. Hayato , I. Heitkamp , D. Henaff , Y. Hino , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , M. C. F. Hooft , K. Hosokawa , J. Hu , A. K. Ichikawa , K. Ieki , M. Ikeda , T. H. Ishida , T. Ishida , M. Ishitsuka , H. Ito , S. Ito , A. Izmaylov , N. Jachowicz , S. J. Jenkins , C. Jesús-Valls , M. Jia , J. J. Jiang , J. Y. Ji , T. P. Jones , P. Jonsson , S. Joshi , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , H. Kakuno , J. Kameda , S. Karpova , V. S. Kasturi , Y. Kataoka , T. Katori , A. Kawabata , Y. Kawamura , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , S. King , V. Kiseeva , J. Kisiel , A. Klustová , L. Kneale , H. Kobayashi , Sota. R Kobayashi , L. Koch , S. Kodama , M. Kolupanova , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , Y. Kudenko , Y. Kudo , A. Kumar Jha , R. Kurjata , V. Kurochka , T. Kutter , L. Labarga , M. Lachat , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , A. Langella , D. H. Langridge , J. -F. Laporte , D. Last , N. Latham , M. Laveder , L. Lavitola , M. Lawe , D. Leon Silverio , S. Levorato , S. V. Lewis , B. Li , C. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , K. K. Mahtani , M. Mandal , S. Manly , A. D. Marino , D. G. R. Martin , D. A. Martinez Caicedo , L. Martinez , 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 , L. Mellet , C. Metelko , M. Mezzetto , S. Miki , V. Mikola , E. W. Miller , A. Minamino , O. Mineev , S. Mine , J. Mirabito , M. Miura , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , A. Muñoz , L. Munteanu , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , K. D. Nakamura , A. Nakano , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , D. T. Nguyen , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , Y. Noguchi , T. Nosek , F. Nova , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , R. Okazaki , W. Okinaga , K. Okumura , T. Okusawa , N. Onda , N. Ospina , L. Osu , N. Otani , Y. Oyama , V. Paolone , J. Pasternak , D. Payne , T. P. D. Peacock , M. Pfaff , L. Pickering , B. Popov , A. J. Portocarrero Yrey , M. Posiadala-Zezula , Y. S. Prabhu , H. Prasad , F. Pupilli , B. Quilain , P. T. Quyen , E. Radicioni , B. Radics , M. A. Ramirez Delgado , R. Ramsden , P. N. Ratoff , M. Reh , G. Reina , C. Riccio , D. W. Riley , E. Rondio , S. Roth , N. Roy , A. Rubbia , L. Russo , A. Rychter , W. Saenz , K. Sakashita , S. Samani , F. Sánchez , 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 , M. Shiozawa , Y. Shiraishi , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , A. J. Speers , R. Spina , A. Srivastava , P. Stowell , Y. Stroke , I. A. Suslov , A. Suzuki , S. Y. Suzuki , M. Tada , S. Tairafune , A. Takeda , Y. Takeuchi , K. Takeya , H. K. Tanaka , H. Tanigawa , A. Teklu , V. V. Tereshchenko , N. Thamm , C. Touramanis , N. Tran , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , M. Varghese , I. Vasilyev , G. Vasseur , E. Villa , U. Virginet , T. Vladisavljevic , T. Wachala , S. -i. Wada , D. Wakabayashi , H. T. Wallace , J. G. Walsh , 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 , K. Yamamoto , T. Yamamoto , C. Yanagisawa , Y. Yang , T. Yano , K. Yasutome , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , R. Zaki , 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

We reexamine the constraints on mixing between electron and muon or tau neutrinos from shock-reheating and r-process nucleosynthesis in supernovae. To this end neutrino flavor evolution is described by nonlinear equations following from a…

Astrophysics · Physics 2009-10-22 G. Sigl

We review the status and the results of reactor neutrino experiments, that toe the cutting edge of neutrino research. Short baseline experiments have provided the measurement of the reactor neutrino spectrum, and are still searching for…

Nuclear Experiment · Physics 2007-05-23 Thierry Lasserre , Henry W. Sobel

The Daya Bay Collaboration has recently observed neutrino oscillations in the nu_e-bar -> nu_e-bar disappearance channel, indicating that sin^2 theta_13 = 0.024 +(-) 0.005 (1 sigma) and theta_13 = 0 is already excluded at the 5.2 sigma…

High Energy Physics - Phenomenology · Physics 2012-05-04 Shun Zhou

It is found that the atmospheric neutrino mixing angle of \theta_{atm} is determined to be \tan\theta_{atm}=Im(B)/Im(C) for B=M_{\nu_e\nu_\mu} and C=M_{\nu_e\nu_\tau}, where M_{ij} is the ij element of M^\dagger_\nu M_\nu with M_\nu as a…

High Energy Physics - Phenomenology · Physics 2014-11-18 Ichiro Aizawa , Masaki Yasue

We discuss a particularly symmetric model of neutrino mixings where, with good accuracy, the atmospheric mixing angle theta_{23} is maximal, theta_{13}=0 and the solar angle satisfies sin^2(theta_{12})=1/3 (Harrison-Perkins-Scott (HPS)…

High Energy Physics - Phenomenology · Physics 2010-04-05 Guido Altarelli , Ferruccio Feruglio

It is proposed that light neutrinos form a triplet in a global SU(3) symmetry in mass eigenstate basis. Assuming that the SU(3)symmetry is broken in the direction (-alambda_{3}+frac{b}/{sqrt{3}}lambda_{8}), and after going to the flavor…

High Energy Physics - Phenomenology · Physics 2008-11-26 Riazuddin

An overview of neutrino-mixing models is presented with emphasis on the types of horizontal flavor and vertical family symmetries that have been invoked. Distributions for the mixing angles of many models are displayed. Ways to…

High Energy Physics - Phenomenology · Physics 2009-05-27 Carl H. Albright

We study a neutrino mass model with $A_4$ discrete flavor symmetry using a type-I seesaw mechanism. The inclusion of extra flavons in our model leads to the deviations from exact tribimaximal mixing pattern resulting in a nonzero…

High Energy Physics - Phenomenology · Physics 2023-07-10 Animesh Barman , Ng. K. Francis , Hrishi Bora

We investigate the effects of a nonzero leptonic mixing angle $\theta_{13}$ on the solar neutrino day-night asymmetry. Using a constant matter density profile for the Earth and well-motivated approximations, we derive analytical expressions…

High Energy Physics - Phenomenology · Physics 2009-11-10 Mattias Blennow , Tommy Ohlsson , Hakan Snellman
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