“…Note that u > 0 in D by the maximum principle. Moreover, as explained above, u is Hölder continuous in R d [21] and thus in particular bounded. Given λ ∈ R, e ∈ ∂B 1 (0) denote v(x) = v λ,e (x) = u(x) − u(x), x ∈ R d , wherex := R λ,e (x) := x − 2(x · e)e + 2λe denotes the reflection of x at T λ,e := ∂H λ,e , H λ,e := {x ∈ R d : x · e > λ}.…”