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Electron antineutrinos are detected in organic liquid scintillator based neutrino experiments by means of the inverse beta decay, producing both a positron and a neutron. The positron may form a bound state together with an electron, called…

Instrumentation and Detectors · Physics 2019-02-20 Mario Schwarz , Sabrina M. Franke , Lothar Oberauer , Miriam D. Plein , Hans Th. J. Steiger , Marc Tippmann

Electron anti-neutrinos are commonly detected in liquid scintillator experiments via inverse beta decay, by looking at the coincidence between the reaction products, neutron and positron. Prior to positron annihilation, an electron-positron…

Instrumentation and Detectors · Physics 2011-02-28 D. Franco , G. Consolati , D. Trezzi

Pulse shape discrimination in liquid scintillator detectors is a well-established technique for the discrimination of heavy particles from light particles. Nonetheless, it is not efficient in the separation of electrons and positrons, as…

Instrumentation and Detectors · Physics 2015-06-16 S. Perasso , G. Consolati , D. Franco , S. Hans , C. Jollet , A. Meregaglia , A. Tonazzo , M. Yeh

Reactor neutrino experiments build large-scale detector systems to detect neutrinos. In liquid scintillator, a neutral bound state of a positron and an electron, named positronium, can be formed. The spin triplet state is called…

Instrumentation and Detectors · Physics 2016-09-15 Ya-Ping Cheng , Liang-Jian Wen , Peng Zhang , Xing-Zhong Cao

Ortho-positronium (o-Ps) formation and decay can replace the annihilation process, when positron interacts in liquid scintillator media. The delay induced by the positronium decay represents either a potential signature for anti-neutrino…

Instrumentation and Detectors · Physics 2013-12-16 G. Consolati , D. Franco , S. Hans , C. Jollet , A. Meregaglia , S. Perasso , A. Tonazzo , M. Yeh

Liquid scintillators are a common choice for neutrino physics experiments, but their capabilities to perform background rejection by scintillation pulse shape discrimination is generally limited in large detectors. This paper describes a…

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 main signature for anti-neutrino detection in reactor and geo-neutrino experiments based on scintillators is provided by the space-time coincidence of positron and neutron produced in the Inverse Beta Decay reaction. Such a signature…

Instrumentation and Detectors · Physics 2015-07-02 G. Consolati , D. Franco , C. Jollet , A. Meregaglia , A. Minotti , S. Perasso , A. Tonazzo

We report first results of a search for the non-zero neutrino mixing angle \theta_{13} from the Double Chooz experiment. Double Chooz aims to measure the mixing angle based on anti-electron-neutrino disappearance as a consequence of…

High Energy Physics - Experiment · Physics 2019-08-13 Tsunayuki Matsubara

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 experiment presents improved measurements of the neutrino mixing angle $\theta_{13}$ using the data collected in 467.90 live days from a detector positioned at an average distance of 1050 m from two reactor cores at the…

High Energy Physics - Experiment · Physics 2015-03-03 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. 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. 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-Castaño , 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. 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 , D. Shrestha , 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 , N. Walsh , H. Watanabe , C. Wiebusch , L. Winslow , M. Wurm , G. Yang , F. Yermia , V. Zimmer

The Double Chooz reactor neutrino experiment will be the next detector to search for a non vanishing theta13 mixing angle with unprecedented sensitivity, which might open the way to unveiling CP violation in the leptonic sector. The…

High Energy Physics - Experiment · Physics 2008-11-26 I. Gil-Botella

Positron lifetime spectra were measured in liquid water at temperatures between 0c and 50c. The long lifetime of ortho-positronium atoms (o-Ps) determined by electron pick-off in molecular substances decreases smoothly by 10% as the…

Other Condensed Matter · Physics 2009-11-10 Katsushige Kotera , Tadashi Saito , Taku Yamanaka

The Double Chooz collaboration presents a measurement of the neutrino mixing angle $\theta_{13}$ using reactor $\overline{\nu}_{e}$ observed via the inverse beta decay reaction in which the neutron is captured on hydrogen. This measurement…

High Energy Physics - Experiment · Physics 2016-02-12 Y. Abe , S. Appel , T. Abrahão , H. Almazan , C. Alt , J. C. dos Anjos , J. C. Barriere , E. Baussan , I. Bekman , M. Bergevin , T. J. C. Bezerra , L. Bezrukov , E. Blucher , T. Brugière , C. Buck , J. Busenitz , A. Cabrera , L. Camilleri , R. Carr , M. Cerrada , E. Chauveau , P. Chimenti , A. P. Collin , J. M. Conrad , J. I. Crespo-Anadón , K. Crum , A. S. Cucoanes , E. Damon , J. V. Dawson , J. Dhooghe , D. Dietrich , Z. Djurcic , M. Dracos , 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 , H. Gomez , L. F. G. Gonzalez , L. Goodenough , M. C. Goodman , N. Haag , T. Hara , J. Haser , D. Hellwig , M. Hofmann , G. A. Horton-Smith , A. Hourlier , M. Ishitsuka , J. Jochum , C. Jollet , F. Kaether , L. N. Kalousis , Y. Kamyshkov , M. Kaneda , 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-Castaño , 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 , D. Navas-Nicolás , P. Novella , L. Oberauer , M. Obolensky , A. Onillon , A. Osborn , C. Palomares , I. M. Pepe , S. Perasso , A. Porta , G. Pronost , J. Reichenbacher , B. Reinhold , M. Röhling , R. Roncin , B. Rybolt , Y. Sakamoto , R. Santorelli , A. C. Schilithz , S. Schönert , S. Schoppmann , M. H. Shaevitz , R. Sharankova , D. Shrestha , V. Sibille , V. Sinev , M. Skorokhvatov , E. Smith , M. Soiron , J. Spitz , A. Stahl , I. Stancu , L. F. F. Stokes , M. Strait , 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 , M. Wurm , G. Yang , F. Yermia , 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 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

One of the features of the triplet state of positronium (ortho-Positronium)atoms is its relatively longer lifetime when compared to the singlet states ofpositronium (para-Positronium) atoms. The most probable decay of ortho-Positronium is…

Instrumentation and Detectors · Physics 2020-02-19 Juhi Raj , Kamil Dilski , Eryk Czerwinski

The Double Chooz reactor neutrino experiment will be the next detector to search for a non vanishing theta(13) mixing angle with unprecedented sensitivity, which might open the way to unveiling CP violation in the leptonic sector. The…

High Energy Physics - Experiment · Physics 2009-05-25 I. Gil-Botella

We discuss the potential of the proposed Double Chooz reactor experiment to measure the neutrino mixing angle $\sin^2 2\theta_{13}$. We especially consider systematical uncertainties and their partial cancellation in a near and far detector…

High Energy Physics - Phenomenology · Physics 2010-02-03 P. Huber , J. Kopp , M. Lindner , M. Rolinec , W. Winter

Double Chooz is a reactor neutrino experiment which investigates the last neutrino mixing angle; theta-13. It is necessary to measure reactor neutrino disappearance with precision 1% or better to detect finite value of theta-13. This…

High Energy Physics - Experiment · Physics 2019-08-13 Fumihiko Suekane
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