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The relatively large measured value of $\theta_{13}$ has opened up the possibility of determining the neutrino mass hierarchy through earth matter effects. Amongst the current accelerator-based experiments only NOvA has a long enough…

High Energy Physics - Phenomenology · Physics 2015-06-12 Anushree Ghosh , Tarak Thakore , Sandhya Choubey

We discuss the optimal setup for a low energy neutrino factory in order to achieve a 5\sigma-discovery of a nonzero mixing angle \theta_{13}, a nonzero CP phase \delta_{CP}, and the mass hierarchy. We explore parent muon energies in the…

High Energy Physics - Phenomenology · Physics 2012-10-08 Amol Dighe , Srubabati Goswami , Shamayita Ray

We discuss unitarity tests of the neutrino mixing (PMNS) matrix. We show that the combination of solar neutrino experiments, medium-baseline and short-baseline reactor antineutrino experiments make it possible to perform the first direct…

High Energy Physics - Experiment · Physics 2013-08-28 X. Qian , C. Zhang , M. Diwan , P. Vogel

The Daya Bay Reactor Antineutrino Experiment reported the first observation of the non-zero neutrino mixing angle $\theta_{13}$ using the first 55 days of data. It has also provided the most precise measurement of $\theta_{13}$ with the…

Instrumentation and Detectors · Physics 2019-08-13 Miao He

The next generation neutrino observatory proposed by the LBNO collaboration will address fundamental questions in particle and astroparticle physics. The experiment consists of a far detector, in its first stage a 20 kt LAr double phase TPC…

High Energy Physics - Phenomenology · Physics 2014-01-21 LBNO Collaboration , S. K. Agarwalla , L. Agostino , M. Aittola , A. Alekou , B. Andrieu , D. Angus , F. Antoniou , A. Ariga , T. Ariga , R. Asfandiyarov , D. Autiero , P. Ballett , I. Bandac , D. Banerjee , G. J. Barker , G. Barr , W. Bartmann , F. Bay , V. Berardi , I. Bertram , O. Bésida , A. M. Blebea-Apostu , A. Blondel , M. Bogomilov , E. Borriello , S. Boyd , I. Brancus , A. Bravar , M. Buizza-Avanzini , F. Cafagna , M. Calin , M. Calviani , M. Campanelli , C. Cantini , O. Caretta , G. Cata-Danil , M. G. Catanesi , A. Cervera , S. Chakraborty , L. Chaussard , D. Chesneanu , F. Chipesiu , G. Christodoulou , J. Coleman , P. Crivelli , T. Davenne , J. Dawson , I. De Bonis , J. De Jong , Y. Déclais , P. Del Amo Sanchez , A. Delbart , C. Densham , F. Di Lodovico , S. Di Luise , D. Duchesneau , J. Dumarchez , I. Efthymiopoulos , A. Eliseev , S. Emery , K. Enqvist , T. Enqvist , L. Epprecht , A. Ereditato , A. N. Erykalov , T. Esanu , A. J. Finch , M. D. Fitton , D. Franco , V. Galymov , G. Gavrilov , A. Gendotti , C. Giganti , B. Goddard , J. J. Gomez , C. M. Gomoiu , Y. A. Gornushkin , P. Gorodetzky , N. Grant , A. Haesler , M. D. Haigh , T. Hasegawa , S. Haug , M. Hierholzer , J. Hissa , S. Horikawa , K. Huitu , J. Ilic , A. N. Ioannisian , A. Izmaylov , A. Jipa , K. Kainulainen , T. Kalliokoski , Y. Karadzhov , J. Kawada , M. Khabibullin , A. Khotjantsev , E. Kokko , A. N. Kopylov , L. L. Kormos , A. Korzenev , S. Kosyanenko , I. Kreslo , D. Kryn , Y. Kudenko , V. A. Kudryavtsev , J. Kumpulainen , P. Kuusiniemi , J. Lagoda , I. Lazanu , J. -M. Levy , R. P. Litchfield , K. Loo , P. Loveridge , J. Maalampi , L. Magaletti , R. M. Margineanu , J. Marteau , C. Martin-Mari , V. Matveev , K. Mavrokoridis , E. Mazzucato , N. McCauley , A. Mercadante , O. Mineev , A. Mirizzi , B. Mitrica , B. Morgan , M. Murdoch , S. Murphy , K. Mursula , S. Narita , D. A. Nesterenko , K. Nguyen , K. Nikolics , E. Noah , Yu. Novikov , H. O'Keeffe , J. Odell , A. Oprima , V. Palladino , Y. Papaphilippou , S. Pascoli , T. Patzak , D. Payne , M. Pectu , E. Pennacchio , L. Periale , H. Pessard , C. Pistillo , B. Popov , P. Przewlocki , M. Quinto , E. Radicioni , Y. Ramachers , P. N. Ratoff , M. Ravonel , M. Rayner , F. Resnati , O. Ristea , A. Robert , E. Rondio , A. Rubbia , K. Rummukainen , R. Sacco , A. Saftoiu , K. Sakashita , J. Sarkamo , F. Sato , N. Saviano , E. Scantamburlo , F. Sergiampietri , D. Sgalaberna , E. Shaposhnikova , M. Slupecki , M. Sorel , N. J. C. Spooner , A. Stahl , D. Stanca , R. Steerenberg , A. R. Sterian , P. Sterian , B. Still , S. Stoica , T. Strauss , J. Suhonen , V. Suvorov , M. Szeptycka , R. Terri , L. F. Thompson , G. Toma , A. Tonazzo , C. Touramanis , W. H. Trzaska , R. Tsenov , K. Tuominen , A. Vacheret , M. Valram , G. Vankova-Kirilova , F. Vanucci , G. Vasseur , F. Velotti , P. Velten , T. Viant , H. Vincke , A. Virtanen , A. Vorobyev , D. Wark , A. Weber , M. Weber , C. Wiebusch , J. R. Wilson , S. Wu , N. Yershov , J. Zalipska , M. Zito

This presentation describes a precision result of the neutrino mixing parameter, $\sin^2 2\theta_{13}$, and the first direct measurement of the antineutrino mass-squared difference $\sin^2(\Delta_{ee}) \equiv \cos^2 \theta_{12} \sin^2…

High Energy Physics - Experiment · Physics 2019-08-13 Bei-Zhen Hu

The prediction of reactor antineutrino spectra will play a crucial role as reactor experiments enter the precision era. The positron energy spectrum of 3.5 million antineutrino inverse beta decay reactions observed by the Daya Bay…

High Energy Physics - Experiment · Physics 2021-07-07 Daya Bay collaboration , F. P. An , A. B. Balantekin , H. R. Band , M. Bishai , S. Blyth , G. F. Cao , J. Cao , J. F. Chang , Y. Chang , H. S. Chen , S. M. Chen , Y. Chen , Y. X. Chen , J. Cheng , Z. K. Cheng , J. J. Cherwinka , M. C. Chu , J. P. Cummings , O. Dalager , F. S. Deng , Y. Y. Ding , M. V. Diwan , T. Dohnal , J. Dove , M. Dvorak , D. A. Dwyer , J. P. Gallo , M. Gonchar , G. H. Gong , H. Gong , W. Q. Gu , J. Y. Guo , L. Guo , X. H. Guo , Y. H. Guo , Z. Guo , R. W. Hackenburg , S. Hans , M. He , K. M. Heeger , Y. K. Heng , A. Higuera , Y. K. Hor , Y. B. Hsiung , B. Z. Hu , J. R. Hu , T. Hu , Z. J. Hu , H. X. Huang , X. T. Huang , Y. B. Huang , P. Huber , D. E. Jaffe , K. L. Jen , X. L. Ji , X. P. Ji , R. A. Johnson , D. Jones , L. Kang , S. H. Kettell , S. Kohn , M. Kramer , T. J. Langford , J. Lee , J. H. C. Lee , R. T. Lei , R. Leitner , J. K. C. Leung , F. Li , J. J. Li , Q. J. Li , S. Li , S. C. Li , W. D. Li , X. N. Li , X. Q. Li , Y. F. Li , Z. B. Li , H. Liang , C. J. Lin , G. L. Lin , S. Lin , J. J. Ling , J. M. Link , L. Littenberg , B. R. Littlejohn , J. C. Liu , J. L. Liu , C. Lu , H. Q. Lu , J. S. Lu , K. B. Luk , X. B. Ma , X. Y. Ma , Y. Q. Ma , C. Marshall , D. A. Martinez Caicedo , K. T. McDonald , R. D. McKeown , Y. Meng , J. Napolitano , D. Naumov , E. Naumova , J. P. Ochoa-Ricoux , A. Olshevskiy , H. -R. Pan , J. Park , S. Patton , J. C. Peng , C. S. J. Pun , F. Z. Qi , M. Qi , X. Qian , N. Raper , J. Ren , C. Morales Reveco , R. Rosero , B. Roskovec , X. C. Ruan , H. Steiner , J. L. Sun , T. Tmej , K. Treskov , W. -H. Tse , C. E. Tull , B. Viren , V. Vorobel , C. H. Wang , J. Wang , M. Wang , N. Y. Wang , R. G. Wang , W. Wang , W. Wang , X. Wang , Y. Wang , Y. F. Wang , Z. Wang , Z. Wang , Z. M. Wang , H. Y. Wei , L. H. Wei , L. J. Wen , K. Whisnant , C. G. White , H. L. H. Wong , E. Worcester , D. R. Wu , F. L. Wu , Q. Wu , W. J. Wu , D. M. Xia , Z. Q. Xie , Z. Z. Xing , J. L. Xu , T. Xu , T. Xue , C. G. Yang , L. Yang , Y. Z. Yang , H. F. Yao , M. Ye , M. Yeh , B. L. Young , H. Z. Yu , Z. Y. Yu , B. B. Yue , S. Zeng , Y. Zeng , L. Zhan , C. Zhang , F. Y. Zhang , H. H. Zhang , J. W. Zhang , Q. M. Zhang , X. T. Zhang , Y. M. Zhang , Y. X. Zhang , Y. Y. Zhang , Z. J. Zhang , Z. P. Zhang , Z. Y. Zhang , J. Zhao , L. Zhou , H. L. Zhuang , J. H. Zou

The Tokai-to-Kamioka-and-Korea (T2KK) neutrino oscillation experiment under examination can have a high sensitivity to determine the neutrino mass hierarchy for a combination of relatively large (\sim 3.0^circ) off-axis angle beam at…

High Energy Physics - Phenomenology · Physics 2009-07-22 Kaoru Hagiwara , Naotoshi Okamura

We propose that reactor experiments could be used to constrain the environment dependence of neutrino mass and mixing parameters, which could be induced due to an acceleron coupling to matter fields. There are several short-baseline reactor…

High Energy Physics - Phenomenology · Physics 2009-11-11 Thomas Schwetz , Walter Winter

The Coulomb enhancement of low energy electrons in nuclear beta decay generates sharp cutoffs in the accompanying antineutrino spectrum at the beta decay endpoint energies. It has been conjectured that these features will interfere with…

High Energy Physics - Phenomenology · Physics 2019-02-15 D. L. Danielson , A. C. Hayes , G. T. Garvey

Beam neutrino oscillation experiments typically employ only one detector at a certain baseline, apart from the near detector that measures the unoscillated neutrino flux at the source. Lately, there have been discussions of having detectors…

High Energy Physics - Phenomenology · Physics 2019-07-03 Minseok Cho , YeolLin ChoeJo , Hye-Sung Lee , Young-Min Lee , Sushant K. Raut

We explore how well reactor antineutrino experiments can constrain or measure the loss of quantum coherence in neutrino oscillations. We assume that decoherence effects are encoded in the size of the neutrino wave-packet, $\sigma$. We find…

High Energy Physics - Phenomenology · Physics 2020-08-24 André de Gouvêa , Valentina De Romeri , Christoph A. Ternes

The three neutrino model has 9 physical parameters, 3 neutrino masses, 3 mixing angles and 3 CP violating phases. Among them, neutrino oscillation experiments can probe 6 parameters: 2 mass squared differences, 3 mixing angles, and 1 CP…

High Energy Physics - Phenomenology · Physics 2009-11-10 Kaoru Hagiwara

In the context of three-neutrino oscillations, we study the possibility of using antineutrinos from nuclear reactors to explore the 10^{-4} {\rm eV^2} < \ms \ltap 8\times 10^{-4} {\rm eV^2} region of the LMA MSW solution of the solar…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. T. Petcov , M. Piai

We discuss the prospects of a very long baseline neutrino oscillation experiment from HIPA to Beijing. The current understanding of neutrino oscillations, both theoretically and experimentally, are summarized. The figure of merits for…

Matter effects modify the mixing and the effective masses of neutrinos in a way which depends on the neutrino mass hierarchy. Consequently, for normal and inverted hierarchies the oscillations and flavor conversion results are different.…

High Energy Physics - Phenomenology · Physics 2013-12-30 Alexei Yu. Smirnov

We underscore the physics advantage of an experiment where neutrinos produced in a beta-beam facility at CERN are observed in a large magnetized iron calorimeter (ICAL) at the India-based Neutrino Observatory (INO). The CERN-INO distance is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sanjib Kumar Agarwalla , Sandhya Choubey , Amitava Raychaudhuri

In the light of the recent Daya Bay result the reactor angle is about 9 degrees, we reconsider the model presented in arXiv:1005.3482 showing that, when all neutrino oscillation parameters are taken at their best fit values of Schwetz et al…

High Energy Physics - Phenomenology · Physics 2015-06-04 D. Meloni , S. Morisi , E. Peinado

The Daya Bay reactor neutrino experiment announced the discovery of a non-zero value of \sin^22\theta_{13} with significance better than 5 \sigma in 2012. The experiment is continuing to improve the precision of \sin^22\theta_{13} and…

High Energy Physics - Experiment · Physics 2019-08-13 Bei-Zhen Hu

Sterile neutrinos are one candidate to explain anomalies in neutrino oscillations. The mass-difference-driving oscillation between flavors can be probed only within specific combinations of baseline and flight energy. For a neutrino whose…

High Energy Physics - Phenomenology · Physics 2013-03-26 S. K. Kang , Y. D. Kim , Y. Ko , K. Siyeon