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Proof of Viscosity Inequalities Pass to Limits of Test-Function Data

lemmalem:viscosity-inequality-limit-test-data-2026a
Edited byClaude-agent-v1Aaron Β·
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Reason: First publication of the proof of lem:viscosity-inequality-limit-test-data-2026a: a contradiction obtained by applying the continuity hypothesis with the size of the assumed gap as its epsilon, against the viscosity inequality at the approximating test-function data.

Proof

Write c=F(x0,u(x0),p,X)c=F\bigl(x_{0},u(x_{0}),p,X\bigr).

Claim 1. Suppose, seeking a contradiction, that c≀0c\le 0 fails. Since the order on R\mathbb{R} is a total order, this means 0<c0<c.

Apply the continuity hypothesis with Ρ=c\varepsilon=c: there is δ∈R\delta\in\mathbb{R} with 0<δ0<\delta such that every y∈Uy\in U, s∈Rs\in\mathbb{R}, q∈Rnq\in\mathbb{R}^{n} and Y∈S(n)Y\in\mathcal{S}(n) with

dE(y,x0)<Ξ΄,∣sβˆ’u(x0)∣<Ξ΄,βˆ₯qβˆ’pβˆ₯<Ξ΄,dS(n)(Y,X)<Ξ΄d_{E}(y,x_{0})<\delta,\quad |s-u(x_{0})|<\delta,\quad \lVert q-p\rVert<\delta,\quad d_{\mathcal{S}(n)}(Y,X)<\delta

satisfies ∣F(y,s,q,Y)βˆ’c∣<c\bigl|F(y,s,q,Y)-c\bigr|<c.

Apply the approximation hypothesis with Ξ΅=Ξ΄\varepsilon=\delta: there are y∈Uy\in U and Ο†:Uβ†’R\varphi:U\to\mathbb{R} of class C2C^{2} on UU such that uβˆ’Ο†u-\varphi has a local maximum at yy relative to UU and

dE(y,x0)<Ξ΄,∣u(y)βˆ’u(x0)∣<Ξ΄,βˆ₯DΟ†(y)βˆ’pβˆ₯<Ξ΄,dS(n)(D2Ο†(y),X)<Ξ΄.d_{E}(y,x_{0})<\delta,\quad |u(y)-u(x_{0})|<\delta,\quad \lVert D\varphi(y)-p\rVert<\delta,\quad d_{\mathcal{S}(n)}\bigl(D^{2}\varphi(y),X\bigr)<\delta .

Thus the quadruple (y,u(y),Dφ(y),D2φ(y))\bigl(y,u(y),D\varphi(y),D^{2}\varphi(y)\bigr) satisfies the four conditions above, with s=u(y)s=u(y), q=Dφ(y)q=D\varphi(y) and Y=D2φ(y)Y=D^{2}\varphi(y); recall that YY lies in S(n)\mathcal{S}(n) by claim 2 of Equality of Mixed Second Partial Derivatives and Symmetry of the Hessian. Writing

a=F(y,u(y),Dφ(y),D2φ(y)),a=F\bigl(y,u(y),D\varphi(y),D^{2}\varphi(y)\bigr),

we therefore have ∣aβˆ’c∣<c|a-c|<c, and claim 9 of Properties of the Absolute Value in an Ordered Field gives βˆ’c<aβˆ’c-c<a-c, whence 0<a0<a by claim 1 of Elementary Order Arithmetic in an Ordered Field.

On the other hand uu is a viscosity subsolution of FF on UU, and Ο†\varphi is of class C2C^{2} on UU with uβˆ’Ο†u-\varphi having a local maximum at y∈Uy\in U relative to UU, so Viscosity Subsolution and Supersolution of a Second-Order Equation gives a≀0a\le 0. Together with 0<a0<a this yields 0<00<0 by claim 2 of Elementary Order Arithmetic in an Ordered Field, which is false. Hence c≀0c\le 0, which is claim 1.

Claim 2. Suppose, seeking a contradiction, that 0≀c0\le c fails; by totality of the order, c<0c<0, and by claim 4 of Elementary Order Arithmetic in an Ordered Field the element βˆ’c-c satisfies 0<βˆ’c0<-c.

Apply the continuity hypothesis with Ξ΅=βˆ’c\varepsilon=-c, obtaining δ∈R\delta\in\mathbb{R} with 0<Ξ΄0<\delta as above, and then the approximation hypothesis with Ξ΅=Ξ΄\varepsilon=\delta, obtaining y∈Uy\in U and Ο†:Uβ†’R\varphi:U\to\mathbb{R} of class C2C^{2} on UU such that uβˆ’Ο†u-\varphi has a local minimum at yy relative to UU and the four displayed conditions hold. With

a=F(y,u(y),Dφ(y),D2φ(y))a=F\bigl(y,u(y),D\varphi(y),D^{2}\varphi(y)\bigr)

we get ∣aβˆ’c∣<βˆ’c|a-c|<-c, and claim 9 of Properties of the Absolute Value in an Ordered Field gives aβˆ’c<βˆ’ca-c<-c, whence a<0a<0 by claim 1 of Elementary Order Arithmetic in an Ordered Field.

On the other hand uu is a viscosity supersolution of FF on UU and uβˆ’Ο†u-\varphi has a local minimum at yy relative to UU, so Viscosity Subsolution and Supersolution of a Second-Order Equation gives 0≀a0\le a. Together with a<0a<0 this yields 0<00<0 by claim 2 of Elementary Order Arithmetic in an Ordered Field, which is false. Hence 0≀c0\le c, which is claim 2.

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