“…However, for the particular choice f = −ϕ, we can define the effective metric h µν = ḡµν = e f +f † g µν , such that with respect to this new metric the condition (3) reduces to the effective Riemannian metricity condition: ∇ λ h αβ = 0. Consequently, the set (M, ḡ, φ = 0, φ † = 0, Bα ) = (M, h, Bα ) receives the name of Riemann frame [19,23,24]. It is important to emphasize here that in both frames geodesics are Weyl invariant and thus these frames are different from the tradictional Jordan and Einstein frames in scalar-tensor theories of gravity [22].…”