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Related papers: Constraints on Oscillation Parameters from $\nu_e$…

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The KARMEN experiment at the spallation neutron source ISIS used \numub from \mup--decay at rest in the search for neutrino oscillations \numubnueb in the appearance mode, with p(\nueb,e+)n as detection reaction of \nueb. In total, 15…

The latest cosmological constraints on the sum of the neutrino masses depend on prior physical assumptions about the mass spectrum. To test the accordance of cosmological and laboratory constraints in the absence of such priors, we…

Cosmology and Nongalactic Astrophysics · Physics 2025-02-14 Willem Elbers , Carlos S. Frenk , Adrian Jenkins , Baojiu Li , Silvia Pascoli

We report on latest results from the Tokai-to-Kamioka experiment studying the disappearance of $\nu_\mu$ and appearance of $\nu_e$ from neutrino oscillation with accelerator generated neutrinos. Thanks to increase in statistics and numerous…

High Energy Physics - Experiment · Physics 2022-02-21 Lukas Berns

Keeping in mind the possibility of large theta(13), which will be soon explored by reactor and accelerator experiments, I formulate a perturbation theory of neutrino oscillation under the ansatz, sin^2(theta_{13}) \simeq Delta…

High Energy Physics - Phenomenology · Physics 2010-02-08 Hisakazu Minakata

An analysis of atmospheric neutrino data from all four run periods of \superk optimized for sensitivity to the neutrino mass hierarchy is presented. Confidence intervals for $\Delta m^2_{32}$, $\sin^2 \theta_{23}$, $\sin^2 \theta_{13}$ and…

High Energy Physics - Experiment · Physics 2018-06-28 Kamiokande Collaboration , K. Abe , C. Bronner , Y. Haga , Y. Hayato , M. Ikeda , K. Iyogi , J. Kameda , Y. Kato , Y. Kishimoto , Ll. Marti , M. Miura , S. Moriyama , M. Nakahata , T. Nakajima , Y. Nakano , S. Nakayama , Y. Okajima , A. Orii , G. Pronost , H. Sekiya , M. Shiozawa , Y. Sonoda , A. Takeda , A. Takenaka , H. Tanaka , S. Tasaka , T. Tomura , R. Akutsu , T. Irvine , T. Kajita , I. Kametani , K. Kaneyuki , Y. Nishimura , K. Okumura , E. Richard , K. M. Tsui , L. Labarga , P. Fernandez , F. d. M. Blaszczyk , J. Gustafson , C. Kachulis , E. Kearns , J. L. Raaf , J. L. Stone , L. R. Sulak , S. Berkman , S. Tobayama , M. Goldhaber , G. Carminati , M. Elnimr , W. R. Kropp , S. Mine , S. Locke , A. Renshaw , M. B. Smy , H. W. Sobel , V. Takhistov , P. Weatherly , K. S. Ganezer , B. L. Hartfiel , J. Hill , N. Hong , J. Y. Kim , I. T. Lim , R. G. Park , T. Akiri , A. Himmel , Z. Li , E. O'Sullivan , K. Scholberg , C. W. Walter , T. Wongjirad , T. Ishizuka , T. Nakamura , J. S. Jang , K. Choi , J. G. Learned , S. Matsuno , S. N. Smith , J. Amey , R. P. Litchfield , W. Y. Ma , Y. Uchida , M. O. Wascko , S. Cao , M. Friend , T. Hasegawa , T. Ishida , T. Ishii , T. Kobayashi , T. Nakadaira , K. Nakamura , Y. Oyama , K. Sakashita , T. Sekiguchi , T. Tsukamoto , KE. Abe , M. Hasegawa , A. T. Suzuki , Y. Takeuchi , T. Yano , T. Hayashino , S. Hirota , K. Huang , K. Ieki , M. Jiang , T. Kikawa , KE. Nakamura , T. Nakaya , N. D. Patel , K. Suzuki , S. Takahashi , R. A. Wendell , L. H. V. Anthony , N. McCauley , A. Pritchard , Y. Fukuda , Y. Itow , G. Mitsuka , M. Murase , F. Muto , T. Suzuki , P. Mijakowski , K. Frankiewicz , J. Hignight , J. Imber , C. K. Jung , X. Li , J. L. Palomino , G. Santucci , C. Vilela , M. J. Wilking , C. Yanagisawa , S. Ito , D. Fukuda , H. Ishino , T. Kayano , A. Kibayashi , Y. Koshio , T. Mori , H. Nagata , M. Sakuda , C. Xu , Y. Kuno , D. Wark , F. Di Lodovico , B. Richards , R. Tacik , S. B. Kim , A. Cole , L. Thompson , H. Okazawa , Y. Choi , K. Ito , K. Nishijima , M. Koshiba , Y. Totsuka , Y. Suda , M. Yokoyama , R. G. Calland , M. Hartz , K. Martens , B. Quilain , C. Simpson , Y. Suzuki , M. R. Vagins , D. Hamabe , M. Kuze , T. Yoshida , M. Ishitsuka , J. F. Martin , C. M. Nantais , P. de Perio , H. A. Tanaka , A. Konaka , S. Chen , L. Wan , Y. Zhang , R. J. Wilkes , A. Minamino

All existing data on neutrino oscillations (including those from the LSND experiment) imply a four neutrino scheme with six different allowed mass patterns. Some of the latter are shown to be disfavored by using a conservative upper bound…

High Energy Physics - Phenomenology · Physics 2009-11-07 Sandip Pakvasa , Probir Roy

We report the results of a search for the neutrinoless double-$\beta$ decay (0$\nu\beta\beta$) of $^{100}$Mo, using the NEMO-3 detector to reconstruct the full topology of the final state events. With an exposure of 34.7 kg.y, no evidence…

The OPERA experiment is designed to search for $\nu_{\mu} \rightarrow \nu_{\tau}$ oscillations in appearance mode i.e. through the direct observation of the $\tau$ lepton in $\nu_{\tau}$ charged current interactions. The experiment has…

High Energy Physics - Experiment · Physics 2014-03-12 N. Agafonova , A. Aleksandrov , A. Anokhina , S. Aoki , A. Ariga , T. Ariga , T. Asada , D. Autiero , A. Ben Dhahbi , A. Badertscher , D. Bender , A. Bertolin , C. Bozza , R. Brugnera , F. Brunet , G. Brunetti , A. Buonaura , S. Buontempo , B. Buettner , L. Chaussard , M. Chernyavsky , V. Chiarella , A. Chukanov , L. Consiglio , N. D'Ambrosio , G. De Lellis , M. De Serio , P. Del Amo Sanchez , A. Di Crescenzo , D. Di Ferdinando , N. Di Marco , S. Dmitrievski , M. Dracos , D. Duchesneau , S. Dusini , T. Dzhatdoev , J. Ebert , A. Ereditato , J. Favier , T. Ferber , G. Ferone , R. A. Fini , T. Fukuda , G. Galati , A. Garfagnini , G. Giacomelli , C. Goellnitz , J. Goldberg , Y. Gornushkin , G. Grella , F. Grianti , M. Guler , C. Gustavino , C. Hagner , K. Hakamata , T. Hara , T. Hayakawa , M. Hierholzer , A. Hollnagel , B. Hosseini , H. Ishida , K. Ishiguro , M. Ishikawa , K. Jakovcic , C. Jollet , C. Kamiscioglu , M. Kamiscioglu , T. Katsuragawa , J. Kawada , H. Kawahara , J. H. Kim , S. H. Kim , M. Kimura , N. Kitagawa , B. Klicek , K. Kodama , M. Komatsu , U. Kose , I. Kreslo , A. Lauria , J. Lenkeit , A. Ljubicic , A. Longhin , P. Loverre , A. Malgin , G. Mandrioli , J. Marteau , T. Matsuo , V. Matveev , N. Mauri , E. Medinaceli , A. Meregaglia , P. Migliozzi , S. Mikado , M. Miyanishi , E. Miyashita , P. Monacelli , M. C. Montesi , K. Morishima , M. T. Muciaccia , N. Naganawa , T. Naka , M. Nakamura , T. Nakano , Y. Nakatsuka , K. Niwa , S. Ogawa , N. Okateva , A. Olshevsky , T. Omura , K. Ozaki , A. Paoloni , B. D. Park , I. G. Park , A. Pastore , L. Patrizii , E. Pennacchio , H. Pessard , C. Pistillo , D. Podgrudkov , N. Polukhina , M. Pozzato , K. Pretzl , F. Pupilli , R. Rescigno , M. Roda , H. Rokujo , T. Roganova , G. Rosa , I. Rostovtseva , A. Rubbia , O. Ryazhskaya , O. Sato , Y. Sato , A. Schembri , W. Schmidt-Parzefal , I. Shakiryanova , T. Shchedrina , A. Sheshukov , H. Shibuya , T. Shiraishi , G. Shoziyoev , S. Simone , M. Sioli , C. Sirignano , G. Sirri , M. Spinetti , L. Stanco , N. Starkov , S. M. Stellacci , M. Stipcevic , T. Strauss , P. Strolin , K. Suzuki , S. Takahashi , M. Tenti , F. Terranova , V. Tioukov , S. Tufanli , P. Vilain , M. Vladimirov , L. Votano , J. L. Vuilleumier , G. Wilquet , B. Wonsak , C. S. Yoon , J. Yoshida , M. Yoshimoto , Y. Zaitsev , S. Zemskova , A. Zghiche

We test the hypothesis of non-radiative neutrinos decay using the latest IceCube data. Namely, we calculate the track-to-shower ratio expected in IceCube for the normal and inverted neutrino mass hierarchy taking into account the…

High Energy Physics - Phenomenology · Physics 2016-01-20 G. Pagliaroli , A. Palladino , F. Vissani , F. L. Villante

We report an updated neutrino mixing angle of $\theta_{13}$ obtained from a complete data sample of the RENO experiment. The experiment has measured the amplitude and frequency of reactor anti-electron-neutrinos ($\bar{\nu}_{e}$)…

We study the transparency $\cal T$ of nuclei for nucleons knocked-out in high-energy semi-inclusive $(e,e'p)$ reactions, using an improved theoretical input, discussed by Nikolaev et al. We establish that neglect of $NN$-correlations…

Nuclear Theory · Physics 2009-10-28 A. S. Rinat , M. F. Taragin

We present constraints on the dark energy equation-of-state parameter, w=P/(rho c^2), using 60 Type Ia supernovae (SNe Ia) from the ESSENCE supernova survey. We derive a set of constraints on the nature of the dark energy assuming a flat…

Standard three-flavor neutrino oscillations have well explained by a wide range of neutrino experiments. However, the anomalous results, such as electron-antineutrino excess seen by LSND and MiniBooNE do not fit the three-flavor paradigm.…

High Energy Physics - Experiment · Physics 2017-10-03 Rijeesh Keloth , Adam Aurisano , Alexander Sousa , Gavin S Davies , Louise Suter , Robert K Plunkett

From the analyses of the recent data of neutrino oscillation experiments (especially the CHOOZ and the Super KAMIOKANDE experiments), we discuss how these data affect the neutrinoless double beta decay ($(\beta \beta)_{0\nu}$) rate and vice…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. Fukuyama , K. Matsuda , H. Nishiura

Here we update the global fit of neutrino oscillations in arXiv:1103.0734 and arXiv:1108.1376 including the recent measurements of reactor antineutrino disappearance reported by the Double Chooz, Daya Bay and RENO experiments, together with…

High Energy Physics - Phenomenology · Physics 2012-10-25 D. V. Forero , M. Tórtola , J. W. F. Valle

The T2K long-baseline neutrino-oscillation experiment accumulated approximately 11.0x10^20 POT (protons on target) data until June 2015. The results of \nu_e appearance as well as \nu_\mu disappearance for 6.57x10^20 POT neutrino beam data…

High Energy Physics - Experiment · Physics 2016-09-07 Yuichi Oyama

Gamma-ray telescopes in orbit around the Earth are searching for evidence of the elusive radionuclide 22Na produced in novae. Previously published uncertainties in the dominant destructive reaction, 22Na(p,g)23Mg, indicated new measurements…

The MiniBooNE experiment at Fermilab reports results from a search for $\bar \nu_\mu \rightarrow \bar \nu_e$ oscillations, using a data sample corresponding to $5.66 \times 10^{20}$ protons on target. An excess of $20.9 \pm 14.0$ events is…

High Energy Physics - Experiment · Physics 2012-08-27 The MiniBooNE Collaboration

We propose an explanation of the NuTeV anomaly in terms of oscillations of electron neutrinos into sterile neutrinos. We derive an approximate average transition probability P(nu_e->nu_s) = 0.21 +- 0.07, which is compatible with other…

High Energy Physics - Phenomenology · Physics 2007-05-23 C. Giunti , M. Laveder

We perform a combined fit to global neutrino oscillation data available as of fall 2016 in the scenario of three-neutrino oscillations and present updated allowed ranges of the six oscillation parameters. We discuss the differences arising…

High Energy Physics - Phenomenology · Physics 2017-02-28 Ivan Esteban , M. C. Gonzalez-Garcia , Michele Maltoni , Ivan Martinez-Soler , Thomas Schwetz