“…As already mentioned in the introduction, the usual definition given in [5] of a weak solution to CO time-fractional diffusion equations, is not suitable for DO time-fractional diffusion equations. Hence we rather follow the strategy implemented in [11] (which is by means of the Laplace transform of tempered distributions), that is recalled below. Let S ′ (R, L 2 (Ω)) := B(S(R, L 2 (Ω)), R) be the space dual to S(R; L 2 (Ω)), put R + := [0, +∞), and denote by S ′ (R + , L 2 (Ω)) := {v ∈ S ′ (R, L 2 (Ω)); supp v ⊂ R + × Ω} the set of distributions in S ′ (R, L 2 (Ω)) that are supported in R + × Ω.…”