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Physics potential of a long-baseline neutrino oscillation experiment using a J-PARC neutrino beam and Hyper-Kamiokande

  • Hyper-Kamiokande Proto-Collaboration
  • The University of Tokyo
  • University of Liverpool
  • Iowa State University
  • University of Bern
  • University of Geneva
  • University of California at Davis
  • University of Warwick
  • Durham University
  • University of Regina
  • University of Oxford
  • Swiss Federal Institute of Technology Zurich
  • University of Edinburgh
  • Polytechnic University of Bari
  • University of British Columbia
  • Royal Holloway University of London
  • York University Toronto
  • Louisiana State University
  • Centre d'Etudes de Saclay
  • University of California at Irvine
  • University of Sheffield
  • Nagoya University
  • Dongshin University
  • National Institute for Nuclear Physics
  • Queen Mary University of London
  • University of Naples Federico II
  • STFC Rutherford Appleton Laboratory
  • University of Washington
  • Laboratoire Leprince-Ringuet
  • Universidad Autónoma de Madrid

Research output: Contribution to journalArticlepeer-review

343 Scopus citations

Abstract

Hyper-Kamiokande will be a next-generation underground water Cherenkov detector with a total (fiducial) mass of 0.99 (0.56) million metric tons, approximately 20 (25) times larger than that of Super-Kamiokande. One of the main goals of Hyper-Kamiokande is the study of CP asymmetry in the lepton sector using accelerator neutrino and anti-neutrino beams. In this paper, the physics potential of a long-baseline neutrino experiment using the Hyper- Kamiokande detector and a neutrino beam from the J-PARC proton synchrotron is presented. The analysis uses the framework and systematic uncertainties derived from the ongoing T2K experiment. With a total exposure of 7.5MW ×107s integrated proton beam power (corresponding to 1.56 × 1022protons on target with a 30 GeV proton beam) to a 2.5° off-axis neutrino beam, it is expected that the leptonic CP phase δCPcan be determined to better than 19 degrees for all possible values of δCP, and CP violation can be established with a statistical significance of more than 3 σ (5 σ) for 76% (58%) of the δCPparameter space. Using both νeappearance and νμ disappearance data, the expected 1 σ uncertainty of sin2Θ23is 0.015(0.006) for sin2Θ23= 0.5(0.45).

Original languageEnglish
Article number053C02
JournalProgress of Theoretical and Experimental Physics
Volume2015
Issue number5
DOIs
StatePublished - 2015

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