Nonlocal porous medium equation and Viscosity solutions: Difference between pages

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(Created page with "''Viscosity solutions'' are a type of weak solutions for elliptic or parabolic fully nonlinear integro-differential equations that is particularly suitable for the [[comparison p...")
 
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The nonlocal porous medium equation of order $\sigma$ is the name currently given to two very different equations, namely
''Viscosity solutions'' are a type of weak solutions for elliptic or parabolic fully nonlinear integro-differential equations that is particularly suitable for the [[comparison principle]] to hold and for stability under uniform limits.


\[ u_t = \nabla \cdot \left ( u \nabla \mathcal{K_\alpha} (u) \right )\]
== Definition ==


\[\mbox{ where } \mathcal{K}_\alpha(u) := C_{n,\alpha}\; u * |x|^{-n+\alpha},\;\; \alpha+2=\sigma \]
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 $\R^n$.


and
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
<blockquote style="background:#DDDDDD;">
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 \[ Iv(x_0) \geq 0. \]
</blockquote>


\[ u_t +(-\Delta)^{s}(u^m) = 0 \]
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
<blockquote style="background:#DDDDDD;">
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 \[ Iv(x_0) \leq 0. \]
</blockquote>


These equations agree when $s=1$ and $m=2$, otherwise they are not only different superficially, they also exhibit extremely different behaviors. They are both fractional order [[Quasilinear equations]].
A continuous function in $\Omega$ which is at the same time a subsolution and a supersolution is said to be a '''viscosity solution'''.
 
The first of the two has the remarkable property (for nonlocal equations at least) that any initial data with compact support remains with compact support for all later times, the opposite is true of the second equation, for which [[instantaneous speed of propagation]] holds.
 
This means that the first model presents us with a [[free boundary problem]]. For this model  global existence and Hölder continuity of weak solutions have been recently obtained <ref name="CV1"/>, there is almost nothing known about the properties of its free boundary, making it a rich source of open questions.
 
For the second equation, both the Cauchy problem and long time behavior have been extensively studied in recent years <ref name="PQRV" /ref>.
 
== References ==
{{reflist|refs=
<ref name="CV1"> {{Citation | last1=Caffarelli | first1=Luis | last2=Vazquez | first2=Juan | title=Nonlinear Porous Medium Flow with Fractional Potential Pressure | url=http://dx.doi.org/10.1007/s00205-011-0420-4 | publisher=Springer Berlin / Heidelberg | year=2011 | journal=Archive for Rational Mechanics and Analysis | issn=0003-9527 | pages=1–29}}</ref>
<ref name="PQRV"> {{Citation | last1=Pablo | first1=Arturo de | last2=Quirós | first2=Fernando | last3=Rodríguez | first3=Ana | last4=Vazquez | first4=Juan Luis | title=A fractional porous medium equation | url=http://www.sciencedirect.com/science/article/pii/S0001870810003130 | doi=DOI: 10.1016/j.aim.2010.07.017 | year=2011 | journal=Advances in Mathematics | issn=0001-8708 | volume=226 | issue=2 | pages=1378–1409}}</ref>
}}
 
[[Category:Quasilinear equations]] [[Category:Evolution equations]] [[Category:Free boundary problems]]

Revision as of 16:06, 2 June 2011

Viscosity solutions are a type of weak solutions for elliptic or parabolic fully nonlinear integro-differential equations that is particularly suitable for the comparison principle to hold and 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

  1. $Iv(x_0)$ is well defined every time $v \in C^2(x_0)$.
  2. $Iv(x_0) \geq Iw(x_0)$ 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.