1. Reactor rate modulation oscillation analysis with two detectors in Double Chooz
- Author
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Christopher Wiebusch, A. Oralbaev, M. C. Goodman, J. C. dos Anjos, M. Kuze, Christian Buck, G. Mention, C. Veyssiere, J. Haser, J.V. Dawson, R. Sharankova, D. Navas-Nicolás, A. Onillon, C. Palomares, H. de Kerret, Anatael Cabrera, J. Maricic, S. Appel, A. Givaudan, M. D. Skorokhvatov, A. Stahl, A. Minotti, R. Milincic, B. Reinhold, K. Kale, L. Scola, G. Yang, Bayarto Lubsandorzhiev, V. V. Sinev, E. Blucher, T. Miletic, L. B. Bezrukov, V. Sibille, Thierry Lasserre, P. Novella, T. Sumiyoshi, M. Obolensky, C. Jollet, Lothar Oberauer, J. Reichenbacher, P. Chimenti, A. Meregaglia, H. P. Lima, C. Lastoria, H. Gomez, E. Kemp, Masaki Ishitsuka, J. Martino, Zelimir Djurcic, Marcos Cerrada, M. Vivier, S. V. Sukhotin, S. Schönert, I. Bekman, J. Busenitz, I. Gil-Botella, S. Wagner, T. Abrahão, Tobias Lachenmaier, O. Corpace, J. M. LoSecco, H. Almazan, C. E. Lane, F. Yermia, C. Mariani, Josef Jochum, Takeo Kawasaki, Junpei Maeda, T. J. C. Bezerra, J. C. Barriere, T. Brugière, Stefan Schoppmann, Manfred Lindner, Luis González, A. Hourlier, I. M. Pepe, D. Kryn, M. Kaneda, J. M. López-Castaño, D. Lhuillier, M. Karakac, A.V. Etenko, B. Viaud, E. Chauveau, I. Stancu, H. Furuta, G. Pronost, F. Suekane, L.F.F. Stokes, D. Hellwig, T. Matsubara, Ying Sun, P. Soldin, T. Hara, Ministerio de Economía y Competitividad (España), Abrahao, T, Almazan, H, dos Anjos, J, Appel, S, Barriere, J, Bekman, I, Bezerra, T, Bezrukov, L, Blucher, E, Brugiere, T, Buck, C, Busenitz, J, Cabrera, A, Cerrada, M, Chauveau, E, Chimenti, P, Corpace, O, Dawson, J, Djurcic, Z, Etenko, A, Furuta, H, Gil-Botella, I, Givaudan, A, Gomez, H, Gonzalez, L, Goodman, M, Hara, T, Haser, J, Hellwig, D, Hourlier, A, Ishitsuka, M, Jochum, J, Jollet, C, Kale, K, Kaneda, M, Karakac, M, Kawasaki, T, Kemp, E, de Kerret, H, Kryn, D, Kuze, M, Lachenmaier, T, Lane, C, Lasserre, T, Lastoria, C, Lhuillier, D, Lima, H, Lindner, M, Lopez-Castano, J, Losecco, J, Lubsandorzhiev, B, Maeda, J, Mariani, C, Maricic, J, Martino, J, Matsubara, T, Mention, G, Meregaglia, A, Miletic, T, Milincic, R, Minotti, A, Navas-Nicolas, D, Novella, P, Oberauer, L, Obolensky, M, Onillon, A, Oralbaev, A, Palomares, C, Pepe, I, Pronost, G, Reichenbacher, J, Reinhold, B, Schonert, S, Schoppmann, S, Scola, L, Sharankova, R, Sibille, V, Sinev, V, Skorokhvatov, M, Soldin, P, Stahl, A, Stancu, I, Stokes, L, Suekane, F, Sukhotin, S, Sumiyoshi, T, Sun, Y, Veyssiere, C, Viaud, B, Vivier, M, Wagner, S, Wiebusch, C, Yang, G, Yermia, F, AstroParticule et Cosmologie (APC (UMR_7164)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université de Paris (UP), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de physique subatomique et des technologies associées (SUBATECH), Université de Nantes - UFR des Sciences et des Techniques (UN UFR ST), Université de Nantes (UN)-Université de Nantes (UN)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-IMT Atlantique Bretagne-Pays de la Loire (IMT Atlantique), Institut Mines-Télécom [Paris] (IMT)-Institut Mines-Télécom [Paris] (IMT), Institut Pluridisciplinaire Hubert Curien (IPHC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Neutrino de Champagne Ardenne (LNCA - UMS 3263), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Centre d'Etudes Nucléaires de Bordeaux Gradignan (CENBG), Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Double Chooz, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité), Université de Nantes (UN)-Université de Nantes (UN)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-IMT Atlantique (IMT Atlantique), Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), and Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
- Subjects
Normalization (statistics) ,model [background] ,Nuclear and High Energy Physics ,Physics - Instrumentation and Detectors ,nuclear reactor [antineutrino/e] ,far detector ,background: model ,FOS: Physical sciences ,mixing angle: measured [neutrino] ,antineutrino/e: nuclear reactor ,CHOOZ ,01 natural sciences ,7. Clean energy ,High Energy Physics - Experiment ,Nuclear physics ,High Energy Physics - Experiment (hep-ex) ,near detector ,Consistency (statistics) ,0103 physical sciences ,Modulation (music) ,[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex] ,ddc:530 ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det] ,010306 general physics ,Neutrino oscillation ,detector [neutrino] ,Physics ,energy: high ,neutrino/e: interaction ,010308 nuclear & particles physics ,Oscillation ,Detector ,oscillation [neutrino] ,Instrumentation and Detectors (physics.ins-det) ,Neutrino Detectors and Telescopes (experiments) ,interaction [neutrino/e] ,Double Chooz ,modulation ,neutrino: detector ,Neutrino detector ,13. Climate action ,S067P13 ,high [energy] ,lcsh:QC770-798 ,neutrino: oscillation ,neutrino: mixing angle: measured ,experimental results - Abstract
A θ 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 of θ and the total background rates without relying on any assumptions on the specific background contributions. The analysis comprises 865 days of data collected in both detectors with at least one reactor in operation. The oscillation results are enhanced by the use of 24.06 days (12.74 days) of reactor-off data in the far (near) detector. The analysis considers the ν¯ interactions up to a visible energy of 8.5 MeV, using the events at higher energies to build a cosmogenic background model considering fast-neutrons interactions and Li decays. The background-model-independent determination of the mixing angle yields sin(2θ) = 0.094 ± 0.017, being the best-fit total background rates fully consistent with the cosmogenic background model. A second oscillation analysis is also performed constraining the total background rates to the cosmogenic background estimates. While the central value is not significantly modified due to the consistency between the reactor-off data and the background estimates, the addition of the background model reduces the uncertainty on θ to 0.015. Along with the oscillation results, the normalization of the anti-neutrino rate is measured with a precision of 0.86%, reducing the 1.43% uncertainty associated to the expectation. [Figure not available: see fulltext.], We acknowledge the support of the CEA, CNRS/IN2P3, the computer centre CC-IN2P3 and LabEx UnivEarthS in France; the Max Planck Gesellschaft, the Deutsche Forschungsgemeinschaft DFG, the Transregional Collaborative Research Center TR27, the excellence cluster “Origin and Structure of the Universe” and the Maier-Leibnitz-Laboratorium Garching in Germany; the Ministry of Education, Culture, Sports, Science and Technology of Japan (MEXT) and the Japan Society for the Promotion of Science (JSPS) in Japan; the Ministerio de Economía, Industria y Competitividad (SEIDI-MINECO) under grants FPA2016-77347-C2-1-P and MdM-2015-0509 in Spain; the Department of Energy and the National Science Foundation and Department of Energy in the United States; the Russian Academy of Science, the Kurchatov Institute and the Russian Foundation for Basic Research (RFBR) in Russia; the Brazilian Ministry of Science, Technology and Innovation (MCTI), the Financiadora de Estudos e Projetos (FINEP), the Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq), the São Paulo Research Foundation (FAPESP) and the Brazilian Network for High Energy Physics (RENAFAE) in Brazil.
- Published
- 2021
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