TheoremBase

The operator has all the properties required by the uniqueness theorem for the Dirichlet problem, by the proposition on the viscous Hamilton-Jacobi operator; the conclusion is that theorem's.

Proof

Let T={t∈R:0≤t}T=\{t\in\mathbb{R}:0\le t\}. Since Ω‾\overline{\Omega} is nonempty and compact by Bounded Open Domain in Euclidean Space (ii) and ff is continuous on Ω‾\overline{\Omega}, A Continuous Function on a Compact Set Admits a Nondecreasing Modulus of Continuity applies with the metric space (Rn,dE)(\mathbb{R}^{n},d_{E}) and K=Ω‾K=\overline{\Omega} and furnishes a modulus of continuity ω:T→R\omega:T\to\mathbb{R} which, by A Continuous Function on a Compact Set Admits a Nondecreasing Modulus of Continuity (i) and A Continuous Function on a Compact Set Admits a Nondecreasing Modulus of Continuity (ii), is nondecreasing and dominates the oscillation of ff in exactly the two senses required of the modulus in The Viscous Hamilton-Jacobi Operator is Continuous, Strictly Proper and Satisfies the Structure Condition. Fix such an ω\omega; the proposition may then be applied with this ω\omega.

By The Viscous Hamilton-Jacobi Operator is Continuous, Strictly Proper and Satisfies the Structure Condition (i) the operator FF is continuous, by The Viscous Hamilton-Jacobi Operator is Continuous, Strictly Proper and Satisfies the Structure Condition (ii) it is strictly proper with constant γ\gamma, and by The Viscous Hamilton-Jacobi Operator is Continuous, Strictly Proper and Satisfies the Structure Condition (iii) the operator FF and this ω\omega satisfy the structure condition of the comparison principle.

The hypotheses of Uniqueness for the Dirichlet Problem for Second-Order Equations are therefore all met, with this FF, this γ\gamma, this ω\omega and the given uu and vv: the domain data are those of Bounded Open Domain in Euclidean Space, the functions uu and vv are continuous on Ω‾\overline{\Omega} as maps into (R,dR)(\mathbb{R},d_{\mathbb{R}}), their restrictions u∣Ωu|_{\Omega} and v∣Ωv|_{\Omega} are viscosity solutions of FF on Ω\Omega, and uu and vv agree on ∂Ω\partial\Omega. That corollary gives u(x)=v(x)u(x)=v(x) for every x∈Ω‾x\in\overline{\Omega}, as required.

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