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Double Chooz experiment will search for a disappearance of the reactor neutrinos from Chooz reactor cores in Ardenne, France, in order to detect the yet unknown neutrino oscillation angle \theta 13. The far detector was completed in 2010…

High Energy Physics - Experiment · Physics 2015-05-30 Masahiro Kuze , for Double Chooz Collaboration

It is now widely accepted that a new middle baseline disappearance reactor neutrino experiment with multiple detectors could provide a clean measurement of the $\theta_{13}$ mixing angle, free from any parameter degeneracies and…

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

The Double Chooz experiment returns to the site of the Chooz experiment with a pair of detectors for a differential neutrino flux measurement, providing sensitivity to sin^2(2theta13) > 0.03. Reaching this goal requires significant…

High Energy Physics - Experiment · Physics 2008-10-17 Charles E. Lane

The Double Chooz Experiment presents an indication of reactor electron antineutrino disappearance consistent with neutrino oscillations. A ratio of 0.944 $\pm$ 0.016 (stat) $\pm$ 0.040 (syst) observed to predicted events was obtained in 101…

High Energy Physics - Experiment · Physics 2013-05-30 Y. Abe , C. Aberle , T. Akiri , J. C. dos Anjos , F. Ardellier , A. F. Barbosa , A. Baxter , M. Bergevin , A. Bernstein , T. J. C. Bezerra , L. Bezrukhov , E. Blucher , M. Bongrand , 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 , S. Cormon , J. I. Crespo-Anadón , M. Cribier , K. Crum , A. Cucoanes , M. V. D'Agostino , E. Damon , J. V. Dawson , S. Dazeley , M. Dierckxsens , D. Dietrich , Z. Djurcic , M. Dracos , V. Durand , Y. Efremenko , M. Elnimr , Y. Endo , A. Etenko , E. Falk , M. Fallot , M. Fechner , F. von Feilitzsch , J. Felde , S. M. Fernandes , D. Franco , A. J. Franke , M. Franke , H. Furuta , R. Gama , I. Gil-Botella , L. Giot , M. Göger-Neff , L. F. G. Gonzalez , M. C. Goodman , J. TM. Goon , D. Greiner , B. Guillon , N. Haag , C. Hagner , T. Hara , F. X. Hartmann , J. Hartnell , T. Haruna , J. Haser , A. Hatzikoutelis , T. Hayakawa , M. Hofmann , G. A. Horton-Smith , M. Ishitsuka , J. Jochum , C. Jollet , C. L. Jones , F. Kaether , L. 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 , Y. Liu , 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 , A. Milzstajn , H. Miyata , D. Motta , Th. A. Mueller , Y. Nagasaka , K. Nakajima , P. Novella , M. Obolensky , L. Oberauer , A. Onillon , A. Osborn , I. Ostrovskiy , C. Palomares , S. J. M. Peeters , I. M. Pepe , S. Perasso , P. Perrin , P. Pfahler , A. Porta , W. Potzel , R. Queval , J. Reichenbacher , B. Reinhold , A. Remoto , D. Reyna , M. Röhling , S. Roth , H. A. Rubin , Y. Sakamoto , R. Santorelli , F. Sato , S. Schönert , S. Schoppmann , U. Schwan , T. Schwetz , M. H. Shaevitz , D. Shrestha , J-L. Sida , V. Sinev , M. Skorokhvatov , E. Smith , J. Spitz , A. Stahl , I. Stancu , M. Strait , A. Stüken , F. Suekane , S. Sukhotin , T. Sumiyoshi , Y. Sun , Z. Sun , R. Svoboda , H. Tabata , N. Tamura , K. Terao , A. Tonazzo , M. Toups , H. H. Trinh Thi , C. Veyssiere , S. Wagner , H. Watanabe , B. White , C. Wiebusch , L. Winslow , M. Worcester , M. Wurm , E. Yanovitch , F. Yermia , K. Zbiri , V. Zimmer

In scintillator detectors, the forward displacement of the neutron in the reaction $\bar\nu_e+p\to e^++n$ provides neutrino directional information as demonstrated by the CHOOZ reactor experiment with 2,500 events. The near detector of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kathrin A. Hochmuth , Manfred Lindner , Georg G. Raffelt

The goal of Double Chooz experiment is a precise measurement of the last unknown mixing angle theta_13 using two identical detectors placed at far and near sites from Chooz reactor cores. The detector is optimized for reactor-neutrino…

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 determined the value of the neutrino oscillation parameter $\theta_{13}$ from an analysis of inverse beta decay interactions with neutron capture on hydrogen. This analysis uses a three times larger fiducial…

High Energy Physics - Experiment · Physics 2013-08-30 Double Chooz Collaboration , 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 , E. Damon , J. V. Dawson , S. Dazeley , D. Dietrich , Z. Djurcic , M. Dracos , V. Durand , J. Ebert , Y. Efremenko , M. Elnimr , A. Erickson , A. Etenko , M. Fallot , M. Fechner , F. von Feilitzsch , J. Felde , S. M. Fernandes , V. Fischer , D. Franco , A. J. Franke , M. Franke , H. Furuta , R. Gama , I. Gil-Botella , L. Giot , M. Göger-Neff , L. F. G. Gonzalez , L. Goodenough , M. C. Goodman , J. TM. Goon , D. Greiner , N. Haag , S. Habib , 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 , 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-Castaño , 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 , M. Meyer , 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 , G. Pronost , J. Reichenbacher , B. Reinhold , A. Remoto , M. Röhling , R. Roncin , S. Roth , B. Rybolt , Y. Sakamoto , R. Santorelli , F. Sato , S. Schönert , 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. Stüken , 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

Neutrino emission from nuclear reactors provides real-time insights into reactor power and fuel evolution, with potential applications in monitoring and nuclear safeguards. Following reactor shutdown, a low-intensity flux of ``residual…

A non zero, surprisingly large value of the third mixing angle $\theta_{13}$ has been measured in reactor neutrino experiments. Currently the most precise measurement of $\sin^2 2\theta_{13}$ has been performed by the Daya Bay experiment…

High Energy Physics - Experiment · Physics 2013-02-12 Rupert Leitner

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 measurement of the last undetermined neutrino mixing angle \theta_{13} is the main goal of the future experimental research on neutrino oscillations. At present, \theta_{13} is only known to be much smaller than the two other mixing…

High Energy Physics - Experiment · Physics 2007-05-23 Dario Motta

We present in this article a detailed quantitative discussion of the measurement of the leptonic mixing angle theta_13 through currently scheduled reactor neutrino oscillation experiments. We thus focus on Double Chooz (Phase I & II), Daya…

High Energy Physics - Experiment · Physics 2012-03-01 Guillaume Mention , Thierry Lasserre , Dario Motta

Precise measurement of the neutrino mixing angle $\theta_{13}$ is the primary goal of the Double Chooz Experiment (DC), which is located in Chooz, France. The inverse beta decay process provides a unique signature of reactor anti-neutrino…

High Energy Physics - Experiment · Physics 2015-11-03 Guang Yang

Two neutrino mixing angles have been measured, and much of the neutrino community is turning its attention to the unmeasured mixing angle, $\quq$, whose best limit comes from the reactor neutrino experiment CHOOZ.\cite{bib:chooz} New two…

High Energy Physics - Experiment · Physics 2007-06-06 Maury Goodman

Double Chooz is a long baseline neutrino oscillation experiment at Chooz, France. The purpose of this experiment is to measure the non-zero neutrino oscillation parameter theta13, a parameter for changing electron neutrinos into other…

High Energy Physics - Experiment · Physics 2014-04-10 Guang Yang

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

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

Recently there has been a lot of interest around the world in the use of nuclear reactors to measure theta 13, the last undetermined angle in the 3-neutrino mixing scenario. In this paper the motivations for theta 13 measurement using short…

High Energy Physics - Experiment · Physics 2007-05-23 F. Dalnoki-Veress