“…Using our fractional divergence and gradient, it is thus possible to write the fractional 𝑝-Laplace like the local 𝑝-Laplace Δ 𝑝 𝑢 = div ⋅(|∇𝑢| 𝑝−2 ∇𝑢). Similar representations have been given in other works such as [6,32,34]. → 1 as 𝑠 → 1, a proof of which can be found in several sources, see, for example, [22] for an elegant proof.…”