3 research outputs found

    Search for n-nbar oscillation in Super-Kamiokande

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    A search for neutron-antineutron (n−nˉn-\bar{n}) oscillation was undertaken in Super-Kamiokande using the 1489 live-day or 2.45×10342.45 \times 10^{34} neutron-year exposure data. This process violates both baryon and baryon minus lepton numbers by an absolute value of two units and is predicted by a large class of hypothetical models where the seesaw mechanism is incorporated to explain the observed tiny neutrino masses and the matter-antimatter asymmetry in the Universe. No evidence for n−nˉn-\bar{n} oscillation was found, the lower limit of the lifetime for neutrons bound in 16{}^{16}O, in an analysis that included all of the significant sources of experimental uncertainties, was determined to be 1.9×10321.9 \times 10^{32}~years at the 90\% confidence level. The corresponding lower limit for the oscillation time of free neutrons was calculated to be 2.7×1082.7 \times 10^8~s using a theoretical value of the nuclear suppression factor of 0.517×10230.517 \times 10^{23}~s−1^{-1} and its uncertainty.Comment: 8 pages, 2 figure

    Search for n-nbar oscillation in Super-Kamiokande

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    A search for neutron-antineutron (n−nˉn-\bar{n}) oscillation was undertaken in Super-Kamiokande using the 1489 live-day or 2.45×10342.45 \times 10^{34} neutron-year exposure data. This process violates both baryon and baryon minus lepton numbers by an absolute value of two units and is predicted by a large class of hypothetical models where the seesaw mechanism is incorporated to explain the observed tiny neutrino masses and the matter-antimatter asymmetry in the Universe. No evidence for n−nˉn-\bar{n} oscillation was found, the lower limit of the lifetime for neutrons bound in 16{}^{16}O, in an analysis that included all of the significant sources of experimental uncertainties, was determined to be 1.9×10321.9 \times 10^{32}~years at the 90\% confidence level. The corresponding lower limit for the oscillation time of free neutrons was calculated to be 2.7×1082.7 \times 10^8~s using a theoretical value of the nuclear suppression factor of 0.517×10230.517 \times 10^{23}~s−1^{-1} and its uncertainty.Comment: 8 pages, 2 figure
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