“…Here, ∆ p u = div(|∇u| p−2 ∇u) is the classical p−Laplacian operator and, for fixed s ∈ (0, 1) and up to a multiplicative positive constant, the fractional p−Laplacian is defined as (−∆) s p u(x) := 2 P.V. Problems driven by operators like L p,s have raised a certain interest in the last few years, both for the mathematical complications that the combination of two so different operators imply and for the wide range of applications, see for instance [5,4,6,11,12,13,14] and the references therein. A common feature of the aforementioned papers is to deal with weak solutions, in contrast with other results existing in the literature where viscosity solutions have been considered, see e.g.…”