“…In particular, recalling that the Riemann–Liouville fractional integral is defined by (e.g., ) taking the relaxation function a ( t ) = t α − 1 /Γ( α ), we have the following fractional integral memory flux law This equation is the starting point for the investigations about fractional thermoelasticity, started with the seminal paper of Povstenko and widely studied in different papers. We refer for example to the recent paper for the fractional advection–diffusion equation and to the monography for a complete review. We underline that, taking together Equation and the energy balance Equation , we obtain a physical derivation of the time‐fractional heat–wave equation, that is where D = k / ρ c , ∂ α + 1 / ∂ t α + 1 is the Caputo fractional derivative and we have used the fact that, for α > 0 and f ( t )∈ C [0, t ], (see , pag.95, Lemma 2.21]) …”