TheoremBase

Viscosity Subsolution, Supersolution and Solution of a Second-Order Equation on a Hilbert Triple

A locally bounded above function u on an open subset U of the large space is a viscosity subsolution of F if, for every δ > 0, every C2C^2 test function φ and every local maximum x̂ of u^-_δ − φ on V∩U, the shifted operator F^-_δ can be made ≤ ε at data in W×R×H×Sym(H) within ε of (x̂, u^-_δ(x̂), Dφ(x̂), D^2φ(x̂)); supersolutions and solutions are defined dually.

Statement

In the setting of Hilbert Triples: Standing Notation and Background, let U⊆HU\subseteq H be nonempty and open in HH, with W=D(A)∩UW=D(A)\cap U and the class C2(U)C^{2}(U) as in Hilbert Triples: Standing Notation and Background (v), let FF be a second-order equation operator on UU relative to (H,V,A)(H,V,A) with δ\delta-shifts Fδ−F^{-}_{\delta} and Fδ+F^{+}_{\delta}, and let u:U→Ru:U\to\mathbb{R}. For each real δ>0\delta>0 the δ\delta-envelopes uδ−u^{-}_{\delta} and uδ+u^{+}_{\delta} of uu are functions on V∩UV\cap U, defined when uu is bounded above, respectively below, near each point of UU; local bounds, local extrema and the classes C2(U)C^{2}(U) are those fixed there, ∥⋅∥\lVert\cdot\rVert is the norm on Sym(H)\mathrm{Sym}(H), and ∣s∣|s| is the absolute value of a real number ss. Since W⊆V∩UW\subseteq V\cap U, the δ\delta-envelopes are defined at every point of WW.

1. (Viscosity subsolution) Suppose that uu is bounded above near each point of UU. The function uu is a viscosity subsolution of FF on UU if for every real δ>0\delta>0, every φ∈C2(U)\varphi\in C^{2}(U), every point x^∈V∩U\hat{x}\in V\cap U at which the function V∩U→RV\cap U\to\mathbb{R} with value uδ−(x)−φ(x)u^{-}_{\delta}(x)-\varphi(x) at xx has a local maximum relative to V∩UV\cap U, and every real ε>0\varepsilon>0, there exist y∈Wy\in W, s∈Rs\in\mathbb{R}, q∈Hq\in H and Y∈Sym(H)Y\in\mathrm{Sym}(H) such that

∣y−x^∣H<ε,∣uδ−(y)−uδ−(x^)∣<ε,∣s−uδ−(x^)∣<ε,|y-\hat{x}|_{H}<\varepsilon,\qquad |u^{-}_{\delta}(y)-u^{-}_{\delta}(\hat{x})|<\varepsilon,\qquad |s-u^{-}_{\delta}(\hat{x})|<\varepsilon, ∣q−Dφ(x^)∣H<ε,∥Y−D2φ(x^)∥<ε,Fδ−(y,s,q,Y)≤ε.|q-D\varphi(\hat{x})|_{H}<\varepsilon,\qquad \lVert Y-D^{2}\varphi(\hat{x})\rVert<\varepsilon,\qquad F^{-}_{\delta}(y,s,q,Y)\le\varepsilon .

2. (Viscosity supersolution) Suppose that uu is bounded below near each point of UU. The function uu is a viscosity supersolution of FF on UU if for every real δ>0\delta>0, every φ∈C2(U)\varphi\in C^{2}(U), every point x^∈V∩U\hat{x}\in V\cap U at which the function V∩U→RV\cap U\to\mathbb{R} with value uδ+(x)−φ(x)u^{+}_{\delta}(x)-\varphi(x) at xx has a local minimum relative to V∩UV\cap U, and every real ε>0\varepsilon>0, there exist y∈Wy\in W, s∈Rs\in\mathbb{R}, q∈Hq\in H and Y∈Sym(H)Y\in\mathrm{Sym}(H) such that

∣y−x^∣H<ε,∣uδ+(y)−uδ+(x^)∣<ε,∣s−uδ+(x^)∣<ε,|y-\hat{x}|_{H}<\varepsilon,\qquad |u^{+}_{\delta}(y)-u^{+}_{\delta}(\hat{x})|<\varepsilon,\qquad |s-u^{+}_{\delta}(\hat{x})|<\varepsilon, ∣q−Dφ(x^)∣H<ε,∥Y−D2φ(x^)∥<ε,−ε≤Fδ+(y,s,q,Y).|q-D\varphi(\hat{x})|_{H}<\varepsilon,\qquad \lVert Y-D^{2}\varphi(\hat{x})\rVert<\varepsilon,\qquad -\varepsilon\le F^{+}_{\delta}(y,s,q,Y) .

3. (Viscosity solution) Suppose that uu is bounded above near each point of UU and bounded below near each point of UU. The function uu is a viscosity solution of FF on UU if it is both a viscosity subsolution and a viscosity supersolution of FF on UU.

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