Abstract <p>Based on the formal theory developed by one of the authors in previous publications, the mechanism of interconvertibility in the system of neutrinos and antineutrinos ν<sub><i>e</i></sub>, ν<sub>μ</sub>, ν<sub>τ</sub>, <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({{\bar {\nu }}_{e}},{{\bar {\nu }}_{\mu }},{{\bar {\nu }}_{\tau }}\)</EquationSource> <!--JETP2570008Skobelev-m1--> </InlineEquation> is considered; this system is treated as an aggregate of <i>N</i> = const identical microscopic objects in <i>N</i><sub><i>S</i></sub> = 6 states with the possibility in principle to explain the “deficit” of solar electron neutrinos. It has also been found that the best agreement with experiment is observed for systems of ν<sub><i>e</i></sub>, ν<sub>μ</sub>, ν<sub>τ</sub> (i.e., for <i>N</i><sub><i>S</i></sub> = 3).</p>

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On the Deficit of Solar Electron Neutrinos

  • V. V. Skobelev,
  • S. V. Kopylov

摘要

Abstract

Based on the formal theory developed by one of the authors in previous publications, the mechanism of interconvertibility in the system of neutrinos and antineutrinos νe, νμ, ντ, \({{\bar {\nu }}_{e}},{{\bar {\nu }}_{\mu }},{{\bar {\nu }}_{\tau }}\) is considered; this system is treated as an aggregate of N = const identical microscopic objects in NS = 6 states with the possibility in principle to explain the “deficit” of solar electron neutrinos. It has also been found that the best agreement with experiment is observed for systems of νe, νμ, ντ (i.e., for NS = 3).