Integral transform

In mathematics, an integral transform is any transform T of the following form:

(Tf)(u) = \int_{t_1}^{t_2} f(t)\, K(t, u)\, dt.

The input of this transform is a function f, and the output is another function Tf.

There are several useful integral transforms. Each transform corresponds to a different choice of the function K, which is called the kernel of the transform.

Table of Integral Transforms
TransformSymbolKernelt1t2
Fourier transform

\mathcal{F}

\frac{e^{iut}}{\sqrt{2 \pi}}

-\infty\,\infty\,
Mellin transform

\mathcal{M}

t^{u-1}\,

0\,\infty\,
Two-sided Laplace transform

\mathcal{B}

e^{-ut}\,

-\infty\,\infty\,
Laplace transform

\mathcal{L}

e^{-ut}\,

0\,\infty\,
Hankel transform

t\,J_\nu(ut)

0\,\infty\,
Abel transform

\frac{t}{\sqrt{t^2-u^2}}

u\,\infty\,
Hilbert transform

\mathcal{H}

\frac{1}{\pi}\frac{1}{u-t}

-\infty\,\infty\,
Identity transform  

\delta (u-t)\,

t_1<u\,t_2>u\,

Although the properties of integral transforms vary widely, they have some properties in common. For example, every integral transform is a linear operator, since the integral is a linear operator, and in fact if the kernel is allowed to be a generalized function then all linear operators are integral transforms (a properly formulated version of this statement is the Schwartz kernel theorem).

See also

External links

Bibliography

See also: Integral transform, Abel transform, Dirac delta function, Fourier transform, Function (mathematics), Generalized function, Hankel transform, Hilbert transform, Kernel (integral operator), Laplace transform