“…At FCC-ee Z-pole energies, the Lorentz boost is larger (βγ ≈ 3) and results in a mean tauonium decay length of L vtx ≈ 30 µm, with counts expected in the tail up to ∼0.1 mm. On the one hand, the diphoton vertex pointing capabilities are coarse, in the 1-cm range for LHC-type calorimeters, unless one uses converted photons and/or high-precision time-of-flight (separating mm distances requires few ps timing resolution) [54]. On the other hand, one could alternatively exploit the T 0 → e + e − γ and T 0 → µ + µ − γ Dalitz decays, with combined branching fraction of O(3%) [11], leading to O(100) or O(20) signal counts at FCC-ee and Belle-II, respectively.…”