- Prime-factor FFT algorithm
The Prime-factor algorithm (PFA), also called the Good-Thomas algorithm (1958/1963), is a
fast Fourier transform (FFT) algorithm that re-expresses thediscrete Fourier transform (DFT) of a size "N" = "N"1"N"2 as a two-dimensional "N"1×"N"2 DFT, but "only" for the case where "N"1 and "N"2 arerelatively prime . These smaller transforms of size "N"1 and "N"2 can then be evaluated by applying PFA recursively or by using some other FFT algorithm.PFA should not be confused with the mixed-radix generalization of the popular Cooley-Tukey algorithm, which also subdivides a DFT of size "N" = "N"1"N"2 into smaller transforms of size "N"1 and "N"2. The latter algorithm can use "any" factors (not necessarily relatively prime), but it has the disadvantage that it also requires extra multiplications by roots of unity called
twiddle factor s, in addition to the smaller transforms. On the other hand, PFA has the disadvantages that it only works for relatively prime factors (e.g. it is useless for power-of-two sizes) and that it requires a more complicated re-indexing of the data based on theChinese Remainder Theorem (CRT). Note, however, that PFA can be combined with mixed-radix Cooley-Tukey, with the former factorizing "N" into relatively prime components and the latter handling repeated factors.PFA is also closely related to the nested
Winograd FFT algorithm , where the latter performs the decomposed "N"1 by "N"2 transform via more sophisticated two-dimensional convolution techniques. Some older papers therefore also call Winograd's algorithm a PFA FFT.(Although the PFA is distinct from the Cooley-Tukey algorithm, it is interesting to note that Good's 1958 work on the PFA was cited as inspiration by Cooley and Tukey in their famous 1965 paper, and there was initially some confusion about whether the two algorithms were different. In fact, it was the only prior FFT work cited by them, as they were not then aware of the earlier research by Gauss and others.)
Algorithm
Recall that the DFT is defined by the formula:
:
The PFA involves a re-indexing of the input and output arrays, which when substituted into the DFT formula transforms it into two nested DFTs (a two-dimensional DFT).
Re-indexing
Suppose that "N" = "N"1"N"2, where "N"1 and "N"2 are relatively prime. In this case, we can define a bijective re-indexing of the input "n" and output "k" by:
::
where "N"1-1 denotes the
modular multiplicative inverse of "N"1 modulo "N"2 and vice-versa for "N"2-1; the indices "k""a" and "n""a" run from 0,...,"N""a"-1 (for "a" = 1, 2). These inverses only exist for relatively prime "N"1 and "N"2, and that condition is also required for the first mapping to be bijective.This re-indexing of "n" is called the "Ruritanian" mapping (also "Good's" mapping), while this re-indexing of "k" is called the "CRT" mapping. The latter refers to the fact that "k" is the solution to the Chinese remainder problem "k" = "k"1 mod "N"1 and "k" = "k"2 mod "N"2.
(One could instead use the Ruritanian mapping for the output "k" and the CRT mapping for the input "n", or various intermediate choices.)
A great deal of research has been devoted to schemes for evaluating this re-indexing efficiently, ideally in-place, while minimizing the number of costly modulo (remainder) operations (Chan, 1991, and references).
DFT re-expression
The above re-indexing is then substituted into the formula for the DFT, and in particular into the product "nk" in the exponent. Because "e"2π"i" = 1, this exponent is evaluated modulo "N": any "N"1"N"2 = "N" cross term in the "nk" product can be set to zero. (Similarly, "X""k" and "x""n" are implicitly periodic in "N", so their subscripts are evaluated modulo "N".) The remaining terms give:
:
The inner and outer sums are simply DFTs of size "N"2 and "N"1, respectively.
(Here, we have used the fact that "N"1-1"N"1 is unity when evaluated modulo "N"2 in the inner sum's exponent, and vice-versa for the outer sum's exponent.)
References
* I. J. Good, "The interaction algorithm and practical Fourier analysis," "J. R. Statist. Soc. B" 20 (2), 361-372 (1958). Addendum, "ibid." 22 (2), 373-375 (1960).
* L. H. Thomas, "Using a computer to solve problems in physics," in "Applications of Digital Computers" (Ginn: Boston, 1963).
* P. Duhamel and M. Vetterli, "Fast Fourier transforms: a tutorial review and a state of the art," "Signal Processing" 19, 259-299 (1990).
* S. C. Chan and K. L. Ho, "On indexing the prime-factor fast Fourier transform algorithm," "IEEE Trans. Circuits and Systems" 38 (8), 951-953 (1991).
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