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Upper limits on perturbations of nuclear decay rates induced by reactor electron antineutrinos
We report the results of an experiment conducted near the High Flux Isotope Reactor of Oak Ridge National Laboratory, designed to address the question of whether a flux of reactor-generated electron antineutrinos (ν¯e) can alter the rates of weak nuclear interaction induced decays of 54Mn, 22Na, and...
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Published in: | Applied radiation and isotopes 2019-07, Vol.149 (C), p.182-199 |
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Main Authors: | , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We report the results of an experiment conducted near the High Flux Isotope Reactor of Oak Ridge National Laboratory, designed to address the question of whether a flux of reactor-generated electron antineutrinos (ν¯e) can alter the rates of weak nuclear interaction induced decays of 54Mn, 22Na, and 60Co. This experiment has small statistical errors but, when systematic uncertainties are included, has null results. Perturbations greater than one part in 104 are excluded at 95% confidence level in β± decay and electron capture processes, in the presence of an antineutrino flux of 3 × 1012 cm−2s−1. The present experimental methods are applicable to a wide range of radionuclides. Improved sensitivity in future experiments can be anticipated as we continue to better understand and reduce the dominant systematic uncertainties.
•We report the results of an experiment conducted near the High Flux Isotope Reactor of Oak Ridge National Laboratory, designed to address the question of whether a flux of reactor-generated electron antineutrinos can alter the rates of weak nuclear interaction induced decays of Mn-54, Na-22, and Co-60.•This experiment has small statistical errors but, when systematic uncertainties are included, has null results.•Perturbations greater than one part in 104 are excluded at 95% confidence level in beta decay and electron capture processes, in the presence of an antineutrino flux of 3 × 1012 cm−2s−1.•The present experimental methods are applicable to a wide range of radionuclides.•Improved sensitivity in future experiments can be anticipated as we continue to better understand and reduce the dominant systematic uncertainties. |
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ISSN: | 0969-8043 1872-9800 |
DOI: | 10.1016/j.apradiso.2019.01.027 |