“…Particularly clean processes are the decays µ → eγ and µ → 3e as well as the coherent µ − → e − conversion in the field of a nucleus, µ − +(A, Z) → e − +(A, Z), the latter being especially sensitive to effective LFV operators involving quarks [2,3]. An immense jump in sensitivity to µ − → e − conversion in nuclei is expected in the near future with experiments such as DeeMe [4,5], COMET [6,7], and Mu2e [8,9]. Since the µ − → e − conversion rate depends on the target nucleus (notably its charge Z), it is possible to differentiate between different LFV effective operators using complementary target nuclei in the event of a positive signal observation [3,[10][11][12][13][14].…”