Lepton flavor changing in neutrinoless ττ decays

preprint1998arXivOpen access

Abstract

Neutrino oscillations, as recently reported by the Super-Kamiokande collaboration, imply that lepton numbers could be violated, and τ±→μ±+ℓ++ℓ−,τ±→μ±+ρ0τ^{\pm}\to μ^{\pm}+\ell^{+}+\ell^{-},τ^{\pm}\toμ^{\pm}+ρ^0 are some typical examples. We point out that in these neutrinoless modes, the GIM cancelation is much milder with only a logarithmic behavior log⁡(mj/mk)\log (m_j /m_k) where mj,km_{j, k} are the neutrino masses. This is in sharp contrast with the vanishingly small amplitude τ±→μ±+γτ^{\pm}\to μ^{\pm}+γ strongly suppressed by the quadratic power (mj2−mk2)/MW2(m_j^2-m_k^2)/ M_{\rm W}^2. In comparison with the hopelessly small branching ratio B(τ±→μ±+γ)≈10−40(τ^{\pm}\to μ^{\pm}+γ)\approx 10^{-40}, the B(τ±→μ±+ℓ++ℓ−)(τ^{\pm}\toμ^{\pm}+\ell^{+}+\ell^{-}) could be larger than 10−1410^{-14}. The latter mode, if measurable, could give one more constraint to the lepton mixing angle sin⁡2θjk\sin 2θ_{jk} and the neutrino mass ratio mj/mkm_j/m_k, and therefore is complementary to neutrino oscillation experiments.

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