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We present a search for signatures of neutrino mixing of electron anti-neutrinos with additional hypothetical sterile neutrino flavors using the Double Chooz experiment. The search is based on data from 5 years of operation of Double Chooz,…

There is an observed deficit of about 6\% in the expected rate of anti-neutrino interactions when averaging over many different reactor experiments. While the significance of the deficit is low (98.6 \% CL), there is speculation that a…

High Energy Physics - Experiment · Physics 2015-01-06 M. Bergevin , C. Grant , R. Svoboda

Double Chooz main target is to measure Theta13 oscillation parameter by comparing reactor neutrino fluxes in two identical detectors located respectively at 400 m and 1 km away from the 2 Chooz reactor cores. The far detector is now under…

Instrumentation and Detectors · Physics 2019-08-13 A. Portaa

The Double Chooz experiment has observed 8,249 candidate electron antineutrino events in 227.93 live days with 33.71 GW-ton-years (reactor power x detector mass x livetime) exposure using a 10.3 cubic meter fiducial volume detector located…

High Energy Physics - Experiment · Physics 2015-06-05 Y. Abe , C. Aberle , J. C. dos Anjos , J. C. Barriere , M. Bergevin , A. Bernstein , T. J. C. Bezerra , L. Bezrukhov , E. Blucher , N. S. Bowden , C. Buck , J. Busenitz , A. Cabrera , E. Caden , L. Camilleri , R. Carr , M. Cerrada , P. -J. Chang , P. Chimenti , T. Classen , A. P. Collin , E. Conover , J. M. Conrad , J. I. Crespo-Anadón , K. Crum , A. Cucoanes , M. V. D'Agostino , E. Damon , J. V. Dawson , S. Dazeley , D. Dietrich , Z. Djurcic , M. Dracos , V. Durand , J. Ebert , Y. Efremenko , M. Elnimr , A. Etenko , M. Fallot , M. Fechner , F. von Feilitzsch , J. Felde , D. Franco , A. J. Franke , M. Franke , H. Furuta , R. Gama , I. Gil-Botella , L. Giot , M. Goger-Neff , L. F. G. Gonzalez , M. C. Goodman , J. TM. Goon , D. Greiner , N. Haag , C. Hagner , T. Hara , F. X. Hartmann , J. Haser , A. Hatzikoutelis , T. Hayakawa , M. Hofmann , G. A. Horton-Smith , A. Hourlier , M. Ishitsuka , J. Jochum , C. Jollet , C. L. Jones , F. Kaether , L. N. Kalousis , Y. Kamyshkov , D. M. Kaplan , T. Kawasaki , G. Keefer , E. Kemp , H. de Kerret , Y. Kibe , T. Konno , D. Kryn , M. Kuze , T. Lachenmaier , C. E. Lane , C. Langbrandtner , T. Lasserre , A. Letourneau , D. Lhuillier , H. P. Lima , M. Lindner , J. M. López-Castanõ , J. M. LoSecco , B. K. Lubsandorzhiev , S. Lucht , D. McKee , J. Maeda , C. N. Maesano , C. Mariani , J. Maricic , J. Martino , T. Matsubara , G. Mention , A. Meregaglia , T. Miletic , R. Milincic , H. Miyata , Th. A. Mueller , Y. Nagasaka , K. Nakajima , P. Novella , M. Obolensky , L. Oberauer , A. Onillon , A. Osborn , I. Ostrovskiy , C. Palomares , I. M. Pepe , S. Perasso , P. Perrin , P. Pfahler , A. Porta , W. Potzel , J. Reichenbacher , B. Reinhold , A. Remoto , M. Rohling , R. Roncin , S. Roth , Y. Sakamoto , R. Santorelli , F. Sato , S. Schonert , S. Schoppmann , T. Schwetz , M. H. Shaevitz , S. Shimojima , D. Shrestha , J. -L. Sida , V. Sinev , M. Skorokhvatov , E. Smith , J. Spitz , A. Stahl , I. Stancu , L. F. F. Stokes , M. Strait , A. Stuken , F. Suekane , S. Sukhotin , T. Sumiyoshi , Y. Sun , R. Svoboda , K. Terao , A. Tonazzo , M. Toups , H. H. Trinh Thi , G. Valdiviesso , C. Veyssiere , S. Wagner , H. Watanabe , B. White , C. Wiebusch , L. Winslow , M. Worcester , M. Wurm , F. Yermia , V. Zimmer

New generation of three reactor neutrino experiments have made definitive measurements of the smallest neutrino mixing angle theta13 in 2012, based on the disappearance of electron antineutrinos. More precise measurements of the mixing…

High Energy Physics - Phenomenology · Physics 2015-05-01 Soo-Bong Kim

The first results from Double Chooz with 100 days of data measured $\sin^2(2\theta_{13}) = 0.086 \pm 0.051$. Backgrounds contribute significantly to the systematic uncertainty budget. Using the incoming neutrino directionality we will…

Instrumentation and Detectors · Physics 2019-08-13 Erica Caden

The question "how small is the lepton mixing angle \theta_{13}?" had a convincing answer in a surprisingly short time, \theta_{13} \simeq 9^{\circ}, a large value comparable to the Chooz limit. It defines a new epoch in the program of…

High Energy Physics - Phenomenology · Physics 2015-06-11 Hisakazu Minakata

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

The disappearance of reactor antineutrinos in the Double Chooz experiment is used to investigate the possibility of neutrino-antineutrino oscillations arising due to the breakdown of Lorentz invariance. We find no evidence for this…

High Energy Physics - Experiment · Physics 2015-06-16 J. S. Diaz , T. Katori , J. Spitz , J. M. Conrad

Triggered by the demand of the IAEA, neutrino physicists in Europe involved with the Double Chooz experiment are studying the potential of neutrino detection to monitor nuclear reactors. In particular a new set of experiments at the ILL is…

Nuclear Experiment · Physics 2011-04-11 M. Cribier

We present a detailed quantitative discussion of the measurement of the leptonic mixing angle $\sin^2 2 \theta_{13}$ with a future reactor neutrino oscillation experiment consisting of a near and far detector. We perform a thorough analysis…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Huber , M. Lindner , T. Schwetz , W. Winter

The Double Chooz reactor-based oscillation experiment searches for an electron antineutrino disappearance signal to investigate the neutrino mass matrix mixing angle theta 13. Double Chooz's reported evidence for this disappearance is…

High Energy Physics - Phenomenology · Physics 2017-08-23 Teppei Katori , Joshua Spitz

The Double Chooz neutrino experiment aims to measure the last unknown neutrino mixing angle theta_13 using two identical detectors positioned at sites both near and far from the reactor cores of the Chooz nuclear power plant. To suppress…

Instrumentation and Detectors · Physics 2015-06-05 D. Dietrich , D. Greiner , J. Jochum , T. Lachenmaier , L. F. F. Stokes , M. Röhling

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

The implications of extra sterile neutrinos for the Double Chooz experiment is expounded. The so-called ``3+2'' mass spectrum with 2 sterile neutrinos mixed with the active ones, is still allowed by the global neutrino data including…

High Energy Physics - Phenomenology · Physics 2007-07-19 Abhijit Bandyopadhyay , Sandhya Choubey

The leptonic mixing angle theta_13 is currently a high-priority topic in the field of neutrino physics, with five experiments under way, searching for neutrino oscillations induced by this angle. We review the phenomenology of theta_13 and…

High Energy Physics - Phenomenology · Physics 2015-03-13 Mauro Mezzetto , Thomas Schwetz

The RENO experiment is a short baseline neutrino experiment in Korea aiming to measure the neutrino mixing angle theta_13 or set limit to sin^2(2 theta_13) less than 0.02. This document describes physics goals, experimental site, detector…

High Energy Physics - Experiment · Physics 2010-03-09 RENO Collaboration , J. K. Ahn

A review of recent measurements of the neutrino mixing angle theta-13 is presented. In the standard parametrisation of three-neutrino mixing this is the last of the three mixing angles to be determined, and is known to be the smallest. The…

High Energy Physics - Experiment · Physics 2012-09-27 R. P. Litchfield

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 neutrino mixing angle theta(13) is at the focus of current neutrino research. From a global analysis of the available oscillation data in a 3-neutrino framework, we previously reported [Phys. Rev. Lett. 101, 141801 (2008)] hints in…

High Energy Physics - Phenomenology · Physics 2013-05-29 G. L. Fogli , E. Lisi , A. Marrone , A. Palazzo , A. M. Rotunno