“…The Crandall-Liggett theorem (see[CL71],[Bar72]) says that −(∂ C 0 E +F ) generates a strong continuous semigroup of ω-quasi contractions on C 0 (Ω). Further, since (∂E) | C 0 is homogeneous of order p − 1, and since(∂E) | C 0 ⊆ ∂ L q Efor all 1 ≤ q ≤ ∞, it follows from[Hau21] that for every u 0 ∈ C 0 (Ω) and g ∈ C((0, T ); C 0 (Ω)) ∩ BV (0, T ; C 0 (Ω)), the mild solution u ∈ C([0, T ]; C 0 (Ω)) of the initial boundary value problem (7.1) is a strong solution and satisfies u ∈ W 1,∞ (δ, T ; C 0 (Ω)), moreover u ∈ C lip ([δ, T ]; C 0 (Ω)) for every 0 < δ < T .In particular, u is a weak solution of the non-local Poisson problem (7.3) with h := g(t) − F (u) − u t (t) ∈ C((0, T ); C 0 ).…”