Decays of the Three Top Contributors to the Reactor ν¯e High-Energy Spectrum, Rb92, Y96gs, and Cs142, Studied with Total Absorption Spectroscopy

B. C. Rasco, M. Wolińska-Cichocka, A. Fijałkowska, K. P. Rykaczewski, M. Karny, R. K. Grzywacz, K. C. Goetz, C. J. Gross, D. W. Stracener, E. F. Zganjar, J. C. Batchelder, J. C. Blackmon, N. T. Brewer, S. Go, B. Heffron, T. King, J. T. Matta, K. Miernik, C. D. Nesaraja, S. V. Paulauskas, M. M. Rajabali, E. H. Wang, J. A. Winger, Y. Xiao, and C. J. Zachary
Phys. Rev. Lett. 117, 092501 – Published 22 August 2016

Abstract

We report total absorption spectroscopy measurements of Rb92, Y96gs, and Cs142 β decays, which are the most important contributors to the high energy ν¯e spectral shape in nuclear reactors. These three β decays contribute 43% of the ν¯e flux near 5.5 MeV emitted by nuclear reactors. This ν¯e energy is particularly interesting due to spectral features recently observed in several experiments including the Daya Bay, Double Chooz, and RENO Collaborations. Measurements were conducted at Oak Ridge National Laboratory by means of proton-induced fission of U238 with on-line mass separation of fission fragments and the Modular Total Absorption Spectrometer. We observe a β-decay pattern that is similar to recent measurements of Rb92, with a ground-state to ground-state β feeding of 91(3)%. We verify the Y96gs ground-state to ground-state β feeding of 95.5(20)%. Our measurements substantially modify the β-decay feedings of Cs142, reducing the β feeding to Ba142 states below 2 MeV by 32% when compared with the latest evaluations. Our results increase the discrepancy between the observed and the expected reactor ν¯e flux between 5 and 7 MeV, the maximum excess increases from 10% to 12%.

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  • Received 4 May 2016

DOI:https://doi.org/10.1103/PhysRevLett.117.092501

© 2016 American Physical Society

Physics Subject Headings (PhySH)

  1. Research Areas
Nuclear Physics

Authors & Affiliations

B. C. Rasco1,2,3,*, M. Wolińska-Cichocka5,2,1, A. Fijałkowska6,3, K. P. Rykaczewski2, M. Karny6,2,1, R. K. Grzywacz3,2,1, K. C. Goetz7,3, C. J. Gross2, D. W. Stracener2, E. F. Zganjar4, J. C. Batchelder8,1, J. C. Blackmon4, N. T. Brewer1,2,3, S. Go3, B. Heffron3,2, T. King3, J. T. Matta2, K. Miernik6,1, C. D. Nesaraja2, S. V. Paulauskas3, M. M. Rajabali9, E. H. Wang10, J. A. Winger11, Y. Xiao3, and C. J. Zachary10

  • 1JINPA, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 2Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37966, USA
  • 4Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803 USA
  • 5Heavy Ion Laboratory, University of Warsaw, PL-02-093 Warsaw, Poland
  • 6Faculty of Physics, University of Warsaw, PL-02-093 Warsaw, Poland
  • 7CIRE Bredesen Center, University of Tennessee, Knoxville, Tennessee 37966, USA
  • 8Department of Nuclear Engineering, University of California, Berkeley, Berkeley California 94720, USA
  • 9Department of Physics, Tennessee Technological University, Cookeville, Tennessee 38505, USA
  • 10Department of Physics and Astronomy, Vanderbilt University, Nashville, Tennessee 37235, USA
  • 11Department of Physics and Astronomy, Mississippi State University, Mississippi State, Mississippi 39762, USA

  • *brasco@utk.edu

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Issue

Vol. 117, Iss. 9 — 26 August 2016

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