“…According to [6,Theorem 1.3], by using vector-valued Calderón-Zygmund theory ( [34]) we infer that the operator defined by (58) can be extended from S λ (0, ∞) ⊗ B to L 1 ((0, ∞), B) as a bounded operator from L 1 ((0, ∞), B) into L 1,∞ ((0, ∞), γ (H, B)) and from H 1 ((0, ∞) γ(H, B)). By proceeding as in the proof of Lemma 2.1 we can conclude that the operator G λ B is bounded from L 1 ((0, ∞) γ(H, B)) and from H 1 ((0, ∞), B) into L 1 ((0, ∞), γ(H, B)).…”