“…It is defined rowisely in the spirit of standard projection-based interpolants π D γ : H s (Ω, R 2 ) → V γ adopted for twoscale Poisson-compatible pairs {V γ , P γin }, with enhanced bubble flux components (see[19,20]). Recalling the definition of π D γ for the single-scale case (23)-(25), the two-scale version becomesπ D γ η = π D,∂ γ η+π D γin (η−π D,∂ γ η), where only the internal interpolantπ D γin has to be updated. A uniform bound for ||Π σ 1,γ τ || H(div,Ω,M) , independent of γ, follows from the same property valid for ||π D γ || H(div,Ω,R 2 ) .…”