“…Thus we must conclude that S, V will either materialize as missing energy or highly boosted lepton-jets [3,25]. For example, in the case of the missing energy mode, the existing LHC searches for Supersymmetry involving jets and/or leptons + MET can be recast for the case of F F production if S, V decay invisibly which then tells us that in such a scenario, e.g., m E(E ) > ∼ 0.90(1.05) TeV [26][27][28] for first/second generation-like isosinglet E (isodoublet E ) and m Q > ∼ 1.3 − 1.5 TeV [3,5], depending on the final state fermion flavor, values which are beyond those directly accessible to the ILC, CEPC or FCC-ee, as we will discuss further below. For third generation-like color-singlet PM the prospects for obtaining comparable constraints are somewhat poorer [29,30].…”