In the setting of Hilbert Triples: Standing Notation and Background, the set H is open in H, since every open ball of (H,dH) is a subset of H; accordingly W=D(A)∩H=D(A) and V∩H=V in the notation of Hilbert Triples: Standing Notation and Background §open-sets, and h is the penalty function. Let F be a second-order equation operator on H relative to (H,V,A), with δ-shifts Fδ− and Fδ+.
Let u,v:H→R and let C∈R satisfy 0≤C, u(x)≤C and −C≤v(x) for every x∈H; then u is bounded above near each point of H and v is bounded below near each point of H by Basic Properties of the δ-Envelopes: Semicontinuity, Duality, Closed Superlevel Sets, Bounds and Monotonicity §bound, so that for each real δ>0 the δ-envelopes uδ− and vδ+ are defined on V. Assume that u is a viscosity subsolution of F on H and that v is a viscosity supersolution of F on H.
Let δ,α,σ,ε,B,G,R∈R satisfy
0<δ<1,1<α,0<σ≤1,0<ε≤1,0≤G,C≤B,
let p,q∈H satisfy ∣p∣H≤σ and ∣q∣H≤σ, and let x^,y^∈V be such that the function V×V→R whose value at (x,y) is
uδ−(x)−vδ+(y)−2α∣x−y∣H2−⟨p,x⟩H−⟨q,y⟩H
attains a maximum at (x^,y^). Assume
δh(x^)≤B,δh(y^)≤B,∣uδ−(x^)∣≤B,∣vδ+(y^)∣≤B,α∣x^−y^∣H≤G,
and
δ2B+1<R,3B+2<R,α+1<R,G+2α<R.
Finally, let λ be a properness constant for F at 3B+2, let (ω1,ω2,ω3) be a structure triple for F at 3B+2, and let ω be a shift modulus for F at (δ,R).
¶ Then there exist x1,y1∈D(A) and τ1,τ2∈R with
∣x1−x^∣H<ε,∣y1−y^∣H<ε,0≤τ1≤(2α+1)ε+σ,0≤τ2≤(2α+1)ε+σ,
such that
λ(uδ−(x^)−vδ+(y^)) ≤ 2λε+2ε+ω(τ1)+ω(τ2)+ω1(∣x1−y1∣H)+ω2(α∣x1−y1∣H2)+ω3(δα2∣x1−y1∣H2).