In mathematics, the fractional Laplacian is an operator, which generalizes the notion of Laplacian spatial derivatives to fractional powers. This operator is often used to generalise certain types of Partial differential equation, two examples are [1] and [2] which both take known PDEs containing the Laplacian and replacing it with the fractional version.
In literature the definition of the fractional Laplacian often varies, but most of the time those definitions are equivalent. The following is a short overview proofen by Kwaśnicki, M in.[3]
Let
p\in[1,infty)
l{X}:=Lp(\Rn)
s\in(0,1)
If we further restrict to
p\in[1,2]
(-\Delta)sf:=
-1 | |
l{F} | |
\xi |
(|\xi|2sl{F}(f))
This definition uses the Fourier transform for
f\inLp(\Rn)
p\in[1,infty)
The Laplacian can also be viewed as a singular integral operator which is defined as the following limit taken in
l{X}
(-\Delta)sf(x)=
4s\Gamma(d/2+s) | |
\pid/2|\Gamma(-s)| |
\lim | |
r\to0+ |
\int\limits | { | |
Rd\setminusBr(x) |
f(x)-f(y) | |
|x-y|d+2s |
dy}
Using the fractional heat-semigroup which is the family of operators
\{Pt\}t
-(-\Delta)sf(x)=
\lim | |
t\to0+ |
Ptf-f | |
t |
It is to note, that the generator is not the fractional Laplacian
(-\Delta)s
-(-\Delta)s
Pt:l{X}\tol{X}
Ptf:=pt*f
where
*
pt:=
-1 | |
l{F} | |
\xi |
-t|\xi|2s | |
(e |
)