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Proposal for an Electron Antineutrino Disappearance Search Using High-Rate Li8 Production and Decay

A. Bungau, A. Adelmann, J. R. Alonso, W. Barletta, R. Barlow, L. Bartoszek, L. Calabretta, A. Calanna, D. Campo, J. M. Conrad, Z. Djurcic, Y. Kamyshkov, M. H. Shaevitz, I. Shimizu, T. Smidt, J. Spitz, M. Wascko, L. A. Winslow, and J. J. Yang
Phys. Rev. Lett. 109, 141802 – Published 4 October 2012
Physics logo See Synopsis: In Search of Sterile Neutrinos

Abstract

This paper introduces an experimental probe of the sterile neutrino with a novel, high-intensity source of electron antineutrinos from the production and subsequent decay of Li8. When paired with an existing 1 kton scintillator-based detector, this Eν=6.4 MeV source opens a wide range of possible searches for beyond standard model physics via studies of the inverse beta decay interaction ν¯e+pe++n. In particular, the experimental design described here has unprecedented sensitivity to ν¯e disappearance at Δm21eV2 and features the ability to distinguish between the existence of zero, one, and two sterile neutrinos.

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  • Received 24 May 2012

DOI:https://doi.org/10.1103/PhysRevLett.109.141802

© 2012 American Physical Society

Synopsis

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In Search of Sterile Neutrinos

Published 4 October 2012

A proposed experiment could, over several years of operation, test the suspicion that the three known flavors of neutrinos sometimes transform into other, undetectable types.

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Authors & Affiliations

A. Bungau1, A. Adelmann2, J. R. Alonso3, W. Barletta3, R. Barlow1, L. Bartoszek4, L. Calabretta5, A. Calanna3, D. Campo3, J. M. Conrad3, Z. Djurcic6, Y. Kamyshkov7, M. H. Shaevitz8, I. Shimizu9, T. Smidt3, J. Spitz3, M. Wascko10, L. A. Winslow3, and J. J. Yang2,3

  • 1University of Huddersfield, Huddersfield HD1 3DH, United Kingdom
  • 2Paul Scherrer Institut, Villigen CH-5232, Switzerland
  • 3Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
  • 4Bartoszek Engineering, Aurora, Illinois 60506, USA
  • 5Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali del Sud, I-95123, Italy
  • 6Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 7University of Tennessee, Knoxville, Tennessee 37996, USA
  • 8Columbia University, New York, New York 10027, USA
  • 9Tohoku University, Sendai 980-8578, Japan
  • 10Imperial College London, London SW7 2AZ, United Kingdom

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Issue

Vol. 109, Iss. 14 — 5 October 2012

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Images

  • Figure 1
    Figure 1
    A schematic of the IsoDAR target and surrounding volumes. The dots represent Li8 (ν¯e) creation points, obtained with 105 60 MeV protons on target simulated. The neutron reflector, shielding, and detector are not shown.Reuse & Permissions
  • Figure 2
    Figure 2
    The expected antineutrino flux and detected event rate in the experimental configuration considered. The antineutrino flux mean energy from Li8 is 6.4 MeV. There are 8.2×105 reconstructed events expected from the 1.29×1023 ν¯e created in the target and sleeve in five years.Reuse & Permissions
  • Figure 3
    Figure 3
    The L/E dependence of two example oscillation signatures after five years of IsoDAR running. The solid curve is the oscillation probability with no smearing in the reconstructed position and energy. The 3+2 example (right) represents oscillations with the global best fit 3+2 parameters from Ref. 32.Reuse & Permissions
  • Figure 4
    Figure 4
    The sensitivity of the IsoDAR experiment to electron antineutrino disappearance in a five-year physics run. The sensitivities for both rate+shape (solid line) and shape only (dashed line) are shown. The μDAR [33] exclusion curve and reactor+gallium [3] allowed region are also shown, along with the expected sensitivities from the PBq source [34] and KATRIN [35] experiments.Reuse & Permissions
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