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Related papers: Theta 13 Determination with Nuclear Reactors

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The Daya Bay reactor experiment has reported the most precise measurement of sin$^{2}2\theta_{13}$ and $\Delta m^{2}_{ee}$ by using a data set with the fully constructed design of 8 antineutrino detectors (ADs). We also report on a new…

High Energy Physics - Phenomenology · Physics 2016-07-26 A. Higuera

Flux is an important source of uncertainties for a reactor neutrino experiment. It is determined from thermal power measurements, reactor core simulation, and knowledge of neutrino spectra of fuel isotopes. Past reactor neutrino experiments…

High Energy Physics - Experiment · Physics 2015-05-27 Jun Cao

Neutrinos are elementary particles in the standard model of particle physics. There are 3 flavors of neutrinos that oscillate among themselves. Their oscillation can be described by a 3$\times$3 unitary matrix, containing three mixing…

High Energy Physics - Experiment · Physics 2015-06-19 Haoqi Lu

The Daya Bay reactor neutrino experiment is the first experiment that measured a non-zero value for the neutrino mixing angle $\theta_{13}$ in 2012. Antineutrinos from six 2.9 GW$_{\text{th}}$ reactors are detected in eight identically…

High Energy Physics - Experiment · Physics 2024-09-24 Jinjing Li

This article describes the setup and performance of the near and far detectors in the Double Chooz experiment. The electron antineutrinos of the Chooz nuclear power plant were measured in two identically designed detectors with different…

Instrumentation and Detectors · Physics 2022-09-14 Double Chooz Collaboration , H. de Kerret , Y. Abe , C. Aberle , T. Abrahão , J. M. Ahijado , T. Akiri , J. M. Alarcón , J. Alba , H. Almazan , J. C. dos Anjos , S. Appel , F. Ardellier , I. Barabanov , J. C. Barriere , E. Baussan , A. Baxter , I. Bekman , M. Bergevin , A. Bernstein , W. Bertoli , T. J. C. Bezerra , L. Bezrukov , C. Blanco , N. Bleurvacq , E. Blucher , H. Bonet , M. Bongrand , N. S Bowden , T. Brugière , C. Buck , M. Buizza Avanzini , J. Busenitz , A. Cabrera , E. Calvo , L. Camilleri , R. Carr , S. Cazaux , J. M. Cela , M. Cerrada , P. J. Chang , P. Charon , E. Chauveau , P. Chimenti , T. Classen , A. P. Collin , E. Conover , J. M Conrad , S. Cormon , O. Corpace , B. Courty , J. I. Crespo-Anadón , M. Cribier , K. Crum , S. Cuadrado , A. Cucoanes , M. D'Agostino , E. Damon , J. V. Dawson , S. Dazeley , M. Dierckxsens , D. Dietrich , Z. Djurcic , F. Dorigo , M. Dracos , V. Durand , Y. Efremekov , M. Elnimr , A. Etenko , E. Falk , M. Fallot , M. Fechner , J. Felde , S. M. Fernandes , C. Fernández-Bedoya , D. Francia , D. Franco , V. Fischer , A. J. Franke , M. Franke , H. Furuta , F. Garcia , J. Garcia , I. Gil-Botella , L. Giot , A. Givaudan , M. Göger-Neff , H. Gomez , L. F. G. Gonzalez , L. Goodenough , M. C. Goodman , J. Goon , B. Gramlich , D. Greiner , A. Guertin , B. Guillon , S. M. Habib , Y. Haddad , T. Hara , F. X. Hartmann , J. Hartnell , J. Haser , A. Hatzikoutelis , D. Hellwig , S. Hervé , R. Hofacker , G. Horton-Smith , A. Hourlier , M. Ishitsuka , K. Jänner , S. Jiménez , J. Jochum , C. Jollet , F. Kaether , K. Kale , L. Kalousis , Y. Kamyshkov , M. Kaneda , D. M. Kaplan , M. Karakac , T. Kawasaki , E. Kemp , Y. Kibe , T. Kirchner , T. Konno , D. Kryn , T. Kutter , M. Kuze , T. Lachenmaier , C. E. Lane , C. Langbrandtner , T. Lasserre , C. Lastoria , L. Latron , C. Leonardo , A. Letourneau , D. Lhuillier , H. P. Lima , M. Lindner , J. M. López-Castaño , J. M. LoSecco , B. Lubsandorzhiev , S. Lucht , J. Maeda , C. N. Maesano , C. Mariani , J. Maricic , F. Marie , J. J. Martinez , J. Martino , T. Matsubara , D. McKee , F. Meigner , G. Mention , A. Meregaglia , J. P. Meyer , T. Miletic , R. Milincic , J. F. Millot , A. Minotti , V. Mirones , H. Miyata , Th. A. Mueller , Y. Nagasaka , K. Nakajima , D. Navas-Nicolás , Y. Nikitenko , P. Novella , L. Oberauer , M. Obolensky , A. Onillon , A. Oralbaev , I. Ostrovskiy , C. Palomares , S. J. M. Peeters , I. M. Pepe , S. Perasso , P. Perrin , P. Pfahler , A. Porta , G. Pronost , J. C. Puras , R. Quéval , J. L. Ramirez , J. Reichenbacher , B. Reinhold , M. Reissfelder , A. Remoto , D. Reyna , I. Rodriguez , M. Röhling , R. Roncin , N. Rudolf , B. Rybolt , Y. Sakamoto , R. Santorelli , F. Sato , U. Schwan , L. Scola , M. Settimo , S. Schönert , S. Schoppmann , L. Scola , M. A. Shaevitz , R. Sharankova , V. Sibille , J. L. Sida , V. Sinev , D. Shrestha , M. Skorokhvatov , P. Soldin , J. Spitz , A. Stahl , I. Stancu , P. Starzynski , M. R. Stock , L. F. F. Stokes , M. Strait , A. Stüken , F. Suekane , S. Sukhotin , T. Sumiyoshi , Y. Sun , Z. Sun , R. Svoboda , H. Tabata , N. Tamura , K. Terao , A. Tonazzo , F. Toral , M. Toups , H. Trinh Thi , F. Valdivia , G. Valdiviesso , N. Vassilopoulos , A. Verdugo , C. Veyssiere , B. Viaud , D. Vignaud , M. Vivier , S. Wagner , C. Wiebusch , B. White , L. Winslow , M. Worcester , M. Wurm , J. Wurtz , G. Yang , J. Yáñez , F. Yermia , K. Zbiri

We study the performance of reactor and superbeam neutrino experiments in the presence of non-standard interactions (NSI). We find that for some non-standard terms, reactor and superbeam experiments would yield conflicting result in the…

High Energy Physics - Phenomenology · Physics 2007-10-11 Joachim Kopp , Manfred Lindner , Toshihiko Ota , Joe Sato

We revisit some of the recent neutrino observations and anomalies in the context of sterile neutrinos. Based on a general parametrization motivated in the presence of sterile neutrinos, the consistency of the MINOS disappearance data with…

High Energy Physics - Phenomenology · Physics 2015-06-03 Bhubanjyoti Bhattacharya , Arun M. Thalapillil , Carlos E. M. Wagner

In this paper, we first calculate the realistic Earth matter effects in the detection of type II supernova neutrinos at the Daya Bay reactor neutrino experiment which is currently under construction. It is found that the Earth matter…

High Energy Physics - Phenomenology · Physics 2009-06-19 Xin-Heng Guo , Ming-Yang Huang , Bing-Lin Young

I discuss why and how powerful is the two-detector setting in neutrino oscillation experiments. I cover three concrete examples: (1) reactor \theta_{13} experiments, (2) T2KK, Tokai-to-Kamioka-Korea two-detector complex for measuring CP…

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

Reactor antineutrinos are used to study neutrino oscillation, search for signatures of non-standard neutrino interactions, and to monitor reactor operation for safeguard applications. The flux and energy spectrum of reactor antineutrinos…

High Energy Physics - Experiment · Physics 2013-05-01 K. M. Heeger , B. R. Littlejohn , H. P. Mumm , M. N. Tobin

We argue that a high precision measurement of the neutrino mixing parameter $\theta_{13}$, within a three neutrino seesaw framework can throw important light on the question of whether the quarks and leptons unify into a single matter at…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. N. Mohapatra

Very soon a new generation of reactor and accelerator neutrino oscillation experiments - Double Chooz, Daya Bay, Reno and T2K - will seek for oscillation signals generated by the mixing parameter theta_13. The knowledge of this angle is a…

High Energy Physics - Experiment · Physics 2014-11-20 R. Battiston , M. Mezzetto , P. Migliozzi , F. Terranova

Among ongoing reactor-based experiments, Double Chooz is unique in obtaining data when the reactor cores are brought down for maintenance. These reactor-off data allow for a clean measurement of the backgrounds of the experiment, thus being…

High Energy Physics - Experiment · Physics 2019-08-13 P. Novella

Conventional reactor neutrino experiments are dissapearance experiments, and thus have less sensitivity to small mixing angles than appearance experiments do. It has been recently shown that future reactor neutrino experiments consisiting…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jose Bernabeu , Sergio Palomares-Ruiz

Neutrino oscillations were discovered by atmospheric and solar neutrino experiments, and have been confirmed by experiments using neutrinos from accelerators and nuclear reactors. It has been found that there are large mixing angles in the…

High Energy Physics - Experiment · Physics 2009-10-23 Trung Le

The long baseline neutrino experiment, T2K, and the reactor experiment, Double Chooz will soon present new data. If we expect $\sin\theta_{13}$ to be 0.1-0.2, which is close to the present experimental upper bound, we should not persist in…

High Energy Physics - Phenomenology · Physics 2011-08-30 Yusuke Shimizu , Morimitsu Tanimoto , Atsushi Watanabe

We study the optimization of a green-field, two-baseline reactor experiment with respect to the sensitivity for electron antineutrino disappearance in search of a light sterile neutrino. We consider both commercial and research reactors and…

High Energy Physics - Phenomenology · Physics 2022-02-16 Jeffrey M. Berryman , Luis A. Delgadillo , Patrick Huber

In recent years the experimental study of neutrino oscillations has much contributed to our knowledge of particle physics by establishing non vanishing neutrino masses and by measuring or constraining the corresponding mixing angles. Within…

High Energy Physics - Phenomenology · Physics 2015-05-30 Davide Meloni

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

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