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Related papers: The Double Chooz antineutrino detectors

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The latest results from the Double Chooz experiment on the neutrino mixing angle $\theta_{13}$ are presented. A detector located at an average distance of 1050 m from the two reactor cores of the Chooz nuclear power plant has accumulated a…

High Energy Physics - Experiment · Physics 2021-02-12 J. I. Crespo-Anadón

The Double Chooz Reactor Neutrino Experiment in France plans to quickly measure the neutrino mixing angle theta-13, or limit it to sin^2 2-theta_13 less than 0.025. The physics reach, experimental site, detector structures, scintillator,…

High Energy Physics - Experiment · Physics 2007-05-23 Maury Goodman Thierry Lasserre

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…

The Double Chooz experiment is meant to search for the neutrino mixing angle theta13 taking advantage of the neutrinos generated at the nuclear power plant of Chooz. Double Chooz relies on neutrino flux measurements at two different…

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

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

We describe a muon track reconstruction algorithm for the reactor anti-neutrino experiment Double Chooz. The Double Chooz detector consists of two optically isolated volumes of liquid scintillator viewed by PMTs, and an Outer Veto above…

Instrumentation and Detectors · Physics 2020-07-08 Double Chooz collaboration , Y. Abe , J. C. dos Anjos , J. C. Barriere , E. Baussan , I. Bekman , M. Bergevin , T. J. C. Bezerra , L. Bezrukov , E. Blucher , C. Buck , J. Busenitz , A. Cabrera , E. Caden , L. Camilleri , R. Carr , M. Cerrada , P. -J. Chang , E. Chauveau , P. Chimenti , A. P. Collin , E. Conover , J. M. Conrad , J. I. Crespo-Anadón , K. Crum , A. Cucoanes , E. Damon , J. V. Dawson , D. Dietrich , Z. Djurcic , M. Dracos , M. Elnimr , A. Etenko , M. Fallot , F. von Feilitzsch , J. Felde , S. M. Fernandes , V. Fischer , D. Franco , M. Franke , H. Furuta , I. Gil-Botella , L. Giot , M. Göger-Neff , L. F. G. Gonzalez , L. Goodenough , M. C. Goodman , C. Grant , N. Haag , T. Hara , J. Haser , M. Hofmann , G. A. Horton-Smith , A. Hourlier , M. Ishitsuka , J. Jochum , C. Jollet , F. Kaether , L. N. Kalousis , Y. Kamyshkov , D. M. Kaplan , T. Kawasaki , E. Kemp , H. de Kerret , D. Kryn , M. Kuze , T. Lachenmaier , C. E. Lane , T. Lasserre , A. Letourneau , D. Lhuillier , H. P. Lima , M. Lindner , J. M. López-Casta no , J. M. LoSecco , B. Lubsandorzhiev , S. Lucht , J. Maeda , C. Mariani , J. Maricic , J. Martino , T. Matsubara , G. Mention , A. Meregaglia , T. Miletic , R. Milincic , A. Minotti , Y. Nagasaka , Y. Nikitenko , P. Novella , M. Obolensky , L. Oberauer , A. Onillon , A. Osborn , C. Palomares , I. M. Pepe , S. Perasso , P. Pfahler , A. Porta , G. Pronost , J. Reichenbacher , B. Reinhold , M. Röhling , R. Roncin , S. Roth , B. Rybolt , Y. Sakamoto , R. Santorelli , A. C. Schilithz , S. Schönert , S. Schoppmann , M. H. Shaevitz , R. Sharankova , S. Shimojima , V. Sibille , 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 , H. H. Trinh Thi , G. Valdiviesso , N. Vassilopoulos , C. Veyssiere , M. Vivier , S. Wagner , H. Watanabe , C. Wiebusch , L. Winslow , M. Wurm , G. Yang , F. Yermia , V. Zimmer

The Double Chooz experiment measures the neutrino mixing angle $\theta_{13}$ by detecting reactor $\bar{\nu}_e$ via inverse beta decay. The positron-neutron space and time coincidence allows for a sizable background rejection, nonetheless…

Instrumentation and Detectors · Physics 2014-10-08 Y. Abe , J. C. dos Anjos , J. C. Barriere , E. Baussan , I. Bekman , M. Bergevin , T. J. C. Bezerra , L. Bezrukov , E. Blucher , C. Buck , J. Busenitz , A. Cabrera , E. Caden , L. Camilleri , R. Carr , M. Cerrada , P. -J. Chang , E. Chauveau , P. Chimenti , A. P. Collin , E. Conover , J. M. Conrad , J. I. Crespo-Anadon , K. Crum , A. S. Cucoanes , E. Damon , J. V. Dawson , J. Dhooghe , D. Dietrich , Z. Djurcic , M. Dracos , M. Elnimr , A. Etenko , M. Fallot , F. von Feilitzsch , J. Felde , S. M. Fernandes , V. Fischer , D. Franco , M. Franke , H. Furuta , I. Gil-Botella , L. Giot , M. Goger-Neff , L. F. G. Gonzalez , L. Goodenough , M. C. Goodman , C. Grant , N. Haag , T. Hara , J. Haser , M. Hofmann , G. A. Horton-Smith , A. Hourlier , M. Ishitsuka , J. Jochum , C. Jollet , F. Kaether , L. N. Kalousis , Y. Kamyshkov , D. M. Kaplan , T. Kawasaki , E. Kemp , H. de Kerret , D. Kryn , M. Kuze , T. Lachenmaier , C. E. Lane , T. Lasserre , A. Letourneau , D. Lhuillier , H. P. Lima , M. Lindner , J. M. Lopez-Castano , J. M. LoSecco , B. Lubsandorzhiev , S. Lucht , J. Maeda , C. Mariani , J. Maricic , J. Martino , T. Matsubara , G. Mention , A. Meregaglia , T. Miletic , R. Milincic , A. Minotti , Y. Nagasaka , Y. Nikitenko , P. Novella , L. Oberauer , M. Obolensky , A. Onillon , A. Osborn , C. Palomares , I. M. Pepe , S. Perasso , P. Pfahler , A. Porta , G. Pronost , J. Reichenbacher , B. Reinhold , M. Rohling , R. Roncin , S. Roth , B. Rybolt , Y. Sakamoto , R. Santorelli , A. C. Schilithz , S. Schonert , S. Schoppmann , M. H. Shaevitz , R. Sharankova , S. Shimojima , D. Shrestha , V. Sibille , 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 , H. H. Trinh Thi , G. Valdiviesso , N. Vassilopoulos , C. Veyssiere , M. Vivier , S. Wagner , N. Walsh , H. Watanabe , C. Wiebusch , L. Winslow , M. Wurm , G. Yang , F. Yermia , V. Zimmer

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

The establishment of the neutrino oscillations phenomenon as a solution to both solar and atmospheric neutrino anomalies had two consequences: a new oscillation mode, labelled $\mathbf{\theta_{13}}$, and the possibility to observe CP…

High Energy Physics - Experiment · Physics 2021-07-27 The Double Chooz Collaboration

Over the course of several decades, organic liquid scintillators have formed the basis for successful neutrino detectors. Gadolinium-loaded liquid scintillators provide efficient background suppression for electron antineutrino detection at…

Instrumentation and Detectors · Physics 2012-06-26 C. Aberle , C. Buck , B. Gramlich , F. X. Hartmann , M. Lindner , S. Schönert , U. Schwan , S. Wagner , H. Watanabe

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

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

There is broad consensus in the worldwide physics community as to the need for a new reactor-neutrino experiment to measure or limit the neutrino mixing angle $\theta_{13}$. The Double Chooz Experiment, planned for operation in the years…

High Energy Physics - Experiment · Physics 2009-11-11 Daniel M. Kaplan

Tremendous progress has been achieved in neutrino oscillation physics during the last few years. However, the smallness of the $\t13$ neutrino mixing angle still remains enigmatic. The current best constraint comes from the CHOOZ reactor…

A $\theta_{13}$ oscillation analysis based on the observed antineutrino rates at the Double Chooz far and near detectors for different reactor power conditions is presented. This approach provides a so far unique simultaneous determination…

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 Double-Chooz experiment goal is to search for a non-vanishing value of the Theta13 neutrino mixing angle. This is the last step to accomplish prior moving towards a new era of precision measurements in the lepton sector. The current…

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

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

Double Chooz is unique among modern reactor-based neutrino experiments studying $\bar \nu_e$ disappearance in that data can be collected with all reactors off. In this paper, we present data from 7.53 days of reactor-off running. Applying…

High Energy Physics - Experiment · Physics 2013-05-30 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-Anadon , 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. 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 , 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. Lopez-Castano , 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

A brief overview of the development of neutrino detectors for long-baseline oscillation experiments at accelerators and reactors is presented. Basic principles and main features of detectors of running accelerator experiments T2K and NOvA…

Instrumentation and Detectors · Physics 2017-06-28 Yury Kudenko