“…Now we would like to recall that any Doss-p-almost periodic function F : [0, ∞) → Y , where p ∈ [1, ∞), can be extended to a Doss-p-almost periodic function F : R → Y defined by F (t) := 0, t < 0 (cf. [46] for the notion used in this paragraph). A similar type of extension can be achieved in a much more general situation; for example, we know that, under certain reasonable conditions, any Doss-(p, φ, F, B, Λ ′ , ρ)-almost periodic function F : Λ × X → Y can be extended to a Doss-(p, φ, F, B, Λ ′ , ρ 1 )-almost periodic function F : R n × X → Y, defined by F (t) := 0, t / ∈ Λ, F (t) := F (t), t ∈ Λ, with ρ 1 := ρ ∪ {(0, 0)} (the corresponding analysis from [46] contains small typographical errors that will be corrected in our forthcoming monograph [42]).…”