  If the magnetic moment of unstable tau neutrinos with the mass of $O$(MeV) is
in the region of $10^{-8}\mu_{B} \lesssim \mu_{\nu_{\tau}} \lesssim
10^{-6}\mu_{B}$, it is compatible with the present experimental and
cosmological bounds.
  It is pointed out here, that if the tau neutrino has such a large magnetic
moment and can oscillate into a neutrino of another flavour the results from
$\nu e$ scattering experiment at LAMPF constrain the tau neutrino mixing angles
to $sin^{2}2\theta_{e \tau} \lesssim 2\times 10^{-6} - 2\times 10^{-2}$ and
$sin^{2}2\theta_{\mu\tau} \lesssim 10^{-6} - 10^{-2}$ depending on the magnetic
moment value in the allowed region.
