Nonlocal operator

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Template:More citations needed Template:Short description In mathematics, a nonlocal operator is a mapping which maps functions on a topological space to functions, in such a way that the value of the output function at a given point cannot be determined solely from the values of the input function in any neighbourhood of any point. An example of a nonlocal operator is the Fourier transform.

Formal definition

Let X be a topological space, Y a set, F(X) a function space containing functions with domain X, and G(Y) a function space containing functions with domain Y. Two functions u and v in F(X) are called equivalent at xX if there exists a neighbourhood N of x such that u(x)=v(x) for all xN. An operator A:F(X)G(Y) is said to be local if for every yY there exists an xX such that Au(y)=Av(y) for all functions u and v in F(X) which are equivalent at x. A nonlocal operator is an operator which is not local.

For a local operator it is possible (in principle) to compute the value Au(y) using only knowledge of the values of u in an arbitrarily small neighbourhood of a point x. For a nonlocal operator this is not possible.

Examples

Differential operators are examples of local operatorsTemplate:Citation needed. A large class of (linear) nonlocal operators is given by the integral transforms, such as the Fourier transform and the Laplace transform. For an integral transform of the form

(Au)(y)=Xu(x)K(x,y)dx,

where K is some kernel function, it is necessary to know the values of u almost everywhere on the support of K(,y) in order to compute the value of Au at y.

An example of a singular integral operator is the fractional Laplacian

(Δ)sf(x)=cd,sdf(x)f(y)|xy|d+2sdy.

The prefactor cd,s:=4sΓ(d/2+s)πd/2|Γ(s)| involves the Gamma function and serves as a normalizing factor. The fractional Laplacian plays a role in, for example, the study of nonlocal minimal surfaces.[1]

Applications

Some examples of applications of nonlocal operators are:

See also

References

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