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Fourier transform on finite groups
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Fourier transform on finite groups : ウィキペディア英語版
Fourier transform on finite groups

In mathematics, the Fourier transform on finite groups is a generalization of the discrete Fourier transform from cyclic to arbitrary finite groups.
==Definitions==
The Fourier transform of a function f : G \rightarrow \mathbb\,
at a representation \varrho : G \rightarrow GL(d_\varrho, \mathbb)\, of G\, is
:
\widehat(\varrho) = \sum_ f(a) \varrho(a).

For each representation \varrho\, of G\,, \widehat(\varrho)\, is a d_\varrho \times d_\varrho\, matrix, where d_\varrho\, is the degree of \varrho\,.
Let \varrho_i\, be a complete set of inequivalent irreducible representations of G. Then the matrix entries of the \varrho_i are mutually orthogonal functions on G. Since the dimension of the transform space is equal to |G|, it follows that \sum_i d_^2=|G|.
The inverse Fourier transform at an element a\, of G\, is given by
:
f(a) = \frac \sum_i d_ \text\left(\varrho_i(a^)\widehat(\varrho_i)\right).


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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