Fourier transform on finite groups
The Fourier transform of a function at a representation of is
For each representation of , is a matrix, where is the degree of .
Let be a complete set of inequivalent irreducible representations of . Then the matrix entries of the are mutually orthogonal functions on . Since the dimension of the transform space is equal to , it follows that .
The inverse Fourier transform at an element of is given by
Transform of a convolution
The convolution of two functions is defined as
The Fourier transform of a convolution at any representation of is given by
For functions , the Plancherel formula states
where are the irreducible representations of
Fourier transform on finite abelian groups
Since the irreducible representations of finite abelian groups are all of degree 1 and hence equal to the irreducible characters of the group, Fourier analysis on finite abelian groups is significantly simplified. For instance, the Fourier transform yields a scalar- and not matrix-valued function.
Furthermore, the irreducible characters of a group may be put in one-to-one correspondence with the elements of the group.
Therefore, we may define the Fourier transform for finite abelian groups as
Note that the right-hand side is simply for the inner product on the vector space of functions from to defined by
The inverse Fourier transform is then given by
A property that is often useful in probability is that the Fourier transform of the uniform distribution is simply where 0 is the group identity and is the Kronecker delta.
This generalization of the discrete Fourier transform is used in numerical analysis. A circulant matrix is a matrix where every column is a cyclic shift of the previous one. Circulant matrices can be diagonalized quickly using the fast Fourier transform, and this yields a fast method for solving systems of linear equations with circulant matrices. Similarly, the Fourier transform on arbitrary groups can be used to give fast algorithms for matrices with other symmetries (Åhlander & Munthe-Kaas 2005). These algorithms can be used for the construction of numerical methods for solving partial differential equations that preserve the symmetries of the equations (Munthe-Kaas 2006).
- Fourier transform
- Discrete Fourier transform
- Representation theory of finite groups
- Character theory
- Terras 1999, p.251
- Åhlander, Krister; Munthe-Kaas, Hans Z. (2005), "Applications of the generalized Fourier transform in numerical linear algebra", BIT 45 (4): 819–850, doi:10.1007/s10543-005-0030-3, MR 2191479.
- Diaconis, P. (1988). Group Representations in Probability and Statistics. Lecture Notes — Monograph Series, Vol. 11. Hayward, California: Institute of Mathematical Statistics.
- Diaconis, P. (1991). "Finite Fourier Methods: Access to Tools." In Probabilistic Combinatorics and its Applications, Proceedings of Symposia in Applied Mathematics, Vol. 44. Bollobás, B., and Chung, F. R. K. (ed.).
- Munthe-Kaas, Hans Z. (2006), "On group Fourier analysis and symmetry preserving discretizations of PDEs", Journal of Physics A 39 (19): 5563–5584, doi:10.1088/0305-4470/39/19/S14, MR 2220776.
- Terras, A. (1999). Fourier Analysis on Finite Groups and Applications. Cambridge: Cambridge University Press.