Plancherel's theorem states that the integral of the squared modulus of a function is equal to the integral of the squared modulus of its spectrum. It corresponds to Parseval's theorem for Fourier series. It is sometimes also known as Rayleigh's theory, since it was first used by Rayleigh (1889) in the investigation of blackbody radiation. In 1910, Plancherel first established conditions under which the theorem holds (Titchmarsh 1924; Bracewell 1965, p. 113).
In other words, let
be a function that is sufficiently smooth and that decays sufficiently quickly near
infinity so that its integrals exist. Further, let
and
be Fourier transform
pairs so that
(1)
| |||
(2)
|
where
denotes the complex conjugate.
Then
(3)
| |||
(4)
| |||
(5)
| |||
(6)
| |||
(7)
| |||
(8)
| |||
(9)
|
where
is the delta function.