Viscosity solutions: Difference between revisions
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''Viscosity solutions'' are a type of weak solutions for elliptic or parabolic fully nonlinear integro-differential equations | ''Viscosity solutions'' are a type of weak solutions for elliptic or parabolic fully nonlinear integro-differential equations based on the notion of the [[comparison principle]]. It is especially suitable for stability under uniform limits. | ||
== Definition == | == Definition == | ||
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A continuous function in $\Omega$ which is at the same time a subsolution and a supersolution is said to be a '''viscosity solution'''. | A continuous function in $\Omega$ which is at the same time a subsolution and a supersolution is said to be a '''viscosity solution'''. | ||
Note that if the operator $I$ happens to be local, the construction of the function $v$ is unnecessary since $Iv(x_0) = I\varphi(x_0)$. Thus for local equations the definition is given evaluating $I\varphi(x_0)$ instead. |
Latest revision as of 09:21, 25 April 2012
Viscosity solutions are a type of weak solutions for elliptic or parabolic fully nonlinear integro-differential equations based on the notion of the comparison principle. It is especially suitable for stability under uniform limits.
Definition
The following is a definition of viscosity solutions for fully nonlinear integro-differential equations of the form $Iu=0$, assuming that the functions involved are defined in the whole space. Other situations can be considered with straight forward modifications in the definition. The nonlocal operator $I$ is not necessarily assumed to be translation invariant. All we assume about $I$ is that it is black box operator such that
- $Iv(x_0)$ is well defined every time $v \in C^2(x_0)$.
- $Iv(x_0) \geq Iw(x_0)$ if $v(x_0)=w(x_0)$ and $v\geq w$ in $\R^n$.
An function $u : \R^n \to \R$, which is upper semicontinuous in $\Omega$, is said to be a viscosity subsolution in $\Omega$ if the following statement holds
For any open $U \subset \Omega$, $x_0 \in U$ and $\varphi \in C^2(U)$ such that $\varphi(x_0)=u(x_0)$ and $\varphi \geq u$ in $U$, we construct the auxiliary function $v$ as \[ v(x) = \begin{cases} \varphi(x) & \text{if } x \in U \\ u(x) & \text{if } x \notin U \end{cases}\] Then, we have the inequality \[ Iv(x_0) \geq 0. \]
An function $u : \R^n \to \R$, which is lower semicontinuous in $\Omega$, is said to be a viscosity supersolution in $\Omega$ if the following statement holds
For any open $U \subset \Omega$, $x_0 \in U$ and $\varphi \in C^2(U)$ such that $\varphi(x_0)=u(x_0)$ and $\varphi \leq u$ in $U$, , we construct the auxiliary function $v$ as \[ v(x) = \begin{cases} \varphi(x) & \text{if } x \in U \\ u(x) & \text{if } x \notin U \end{cases}\] Then, we have the inequality \[ Iv(x_0) \leq 0. \]
A continuous function in $\Omega$ which is at the same time a subsolution and a supersolution is said to be a viscosity solution.
Note that if the operator $I$ happens to be local, the construction of the function $v$ is unnecessary since $Iv(x_0) = I\varphi(x_0)$. Thus for local equations the definition is given evaluating $I\varphi(x_0)$ instead.