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Indication of reactor ν ̄e disappearance in the double chooz experiment

  • 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
  • Tokyo Institute of Technology
  • Max-Planck-Institut für Kernphysik
  • Université Paris Diderot
  • Commissariat A l'Énergie Atomique et Aux Énergies Alternatives, Centre de Saclay, IRFU
  • Centro Brasileiro de Pesquisas Físicas
  • University of Sussex
  • University of California, Davis
  • Lawrence Livermore National Laboratory
  • Tohoku University
  • Institute for Nuclear Research of the Russian Academy of Sciences
  • University of Chicago
  • University of Alabama
  • Drexel University
  • Columbia University
  • CIEMAT Energy Department
  • Kansas State University
  • UFABC
  • Massachusetts Institute of Technology
  • SUBATECH, CNRS/IN2P3, Ecole des Mines de Nantes
  • Argonne National Laboratory
  • Laboratoire Neutrino de Champagne Ardenne
  • University of Tübingen
  • Universite de Strasbourg
  • University of Tennessee
  • Tokyo Metropolitan University
  • National Research Centre "Kurchatov Institute"
  • Technical University of Munich
  • University of Campinas
  • Universität Hamburg
  • Kobe University
  • Niigata University
  • Illinois Institute of Technology
  • University of Notre Dame
  • RWTH Aachen University
  • Hiroshima Institute of Technology
  • Tohoku Gakuin University

Research output: Contribution to journalArticlepeer-review

1202 Scopus citations

Abstract

The Double Chooz experiment presents an indication of reactor electron antineutrino disappearance consistent with neutrino oscillations. An observed-to-predicted ratio of events of 0.944±0.016(stat)±0. 040(syst) was obtained in 101 days of running at the Chooz nuclear power plant in France, with two 4.25GW th reactors. The results were obtained from a single 10m3 fiducial volume detector located 1050 m from the two reactor cores. The reactor antineutrino flux prediction used the Bugey4 flux measurement after correction for differences in core composition. The deficit can be interpreted as an indication of a nonzero value of the still unmeasured neutrino mixing parameter sin22θ 13. Analyzing both the rate of the prompt positrons and their energy spectrum, we find sin22θ 13=0.086±0.041(stat)±0.030(syst) , or, at 90% C.L., 0.017< sin22θ 13<0.16.

Original languageEnglish
Article number131801
JournalPhysical Review Letters
Volume108
Issue number13
DOIs
StatePublished - 28 Mar 2012

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