The cross-correlation theorem expresses the Fourier transform of a cross-correlation as the
product of the complex conjugate of one Fourier
transform with the other. Let denote the cross-correlation
of functions
and
. Then
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(1)
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(2)
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(3)
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(4)
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(5)
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(6)
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(7)
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where
denotes the Fourier transform,
,
, and
is the complex conjugate.
The inverse Fourier transform gives
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(8)
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(9)
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The oscillatory integral over in the derivation is interpreted as a distribution,
giving the delta function
, rather than as a convergent ordinary integral.
Applying a Fourier transform on each side gives
the cross-correlation theorem,
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(10)
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If ,
then the cross-correlation theorem reduces to the Wiener-Khinchin
theorem.