Abstract
The different time variations of solar-neutrino observations in the $^{37}\mathrm{Cl}$ and Kamiokande II experiments are accounted for by postulating a sizable contribution from an additional electromagnetic interaction via a neutrino magnetic moment in the Kamiokande II detector. Based on the combined effects of weak and electromagnetic interactions of neutrinos, this discrepancy in the time variation provides a range of allowed values for a Dirac-type neutrino magnetic moment, $4.0l{\ensuremath{\mu}}_{{\ensuremath{\nu}}_{e}}l7.9\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}10}$${\mathrm{\ensuremath{\mu}}}_{\mathit{B}}$ at 95% C.L. (in units of Bohr magneton), assuming that the solar-neutrino deficit is uniform in neutrino energy.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.