A generalization of pde's from a Krylov point of view

preprint2020arXivOpen access

Abstract

We introduce and investigate the notion of a `generalized equation' of the form f(D2u)=0f(D^2 u)=0, based on the notions of subequations and Dirichlet duality. Precisely, a subset H⊂Sym2(Rn){\mathbb H}\subset {\rm Sym}^2({\mathbb R}^n) is a generalized equation if it is an intersection H=E∩(−G~){\mathbb H} = {\mathbb E}\cap (-\widetilde{\mathbb G}) where E{\mathbb E} and G{\mathbb G} are subequations and G~\widetilde{\mathbb G} is the subequation dual to G{\mathbb G}. We utilize a viscosity definition of `solution' to H{\mathbb H}. The mirror of H{\mathbb H} is defined by H∗≡G∩(−E~){\mathbb H}^* \equiv {\mathbb G}\cap (-\widetilde {\mathbb E}). One of the main results here concerns the Dirichlet problem on arbitrary bounded domains Ω⊂RnΩ\subset {\mathbb R}^n for solutions to H{\mathbb H} with prescribed boundary function φ∈C(∂Ω)φ\in C(\partial Ω). We prove that: (A) Uniqueness holds   ⟺  \iff H{\mathbb H} has no interior, and (B) Existence holds   ⟺  \iff H∗{\mathbb H}^* has no interior. For (B) the appropriate boundary convexity of ∂Ω\partial Ω must be assumed. Many examples of generalized equations are discussed, including the constrained Laplacian, the twisted Monge-Ampère equation, and the C1,1C^{1,1}-equation. The closed sets H{\mathbb H} which can be written as generalized equations are intrinsically characterized. For such an H{\mathbb H} the set of subequation pairs with H=E∩(−G~){\mathbb H} = {\mathbb E}\cap (-\widetilde{\mathbb G}) is partially ordered, and there is a canonical least element, contained in all others. Harmonics for the canonical equation are harmonic for all others giving H{\mathbb H}. A general form of the main theorem, which holds on any manifold, is also established.

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