Abstract

We study μ−eμ- e conversion with sequential four generations. A large mass for the fourth generation neutrino can enhance the conversion rate by orders of magnitude. We compare constraints obtained from μ−eμ- e conversion using experimental bounds on various nuclei with those from μ→eγμ\to e γ and μ→eeˉeμ\to e\bar e e. We find that the current bound from μ−eμ- e conversion with Au puts the most stringent constraint in this model. The relevant flavor changing parameter λμe=Vμ4∗Ve4λ_{μe} = V^*_{μ4}V_{e4}^{} is constrained to be less than 1.6×10−51.6\times 10^{-5} for the fourth generation neutrino mass larger than 100 GeV. Implications for future μ−eμ-e conversion, μ→eγμ\to eγ and μ→eeˉeμ\to e\bar e e experiments are discussed.

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