Node:1d Real-even DFTs (DCTs), Next:1d Real-odd DFTs (DSTs), Previous:The 1d Real-data DFT, Up:What FFTW Really Computes
The Real-even DFTs in FFTW are exactly equivalent to the unnormalized forward (and backward) DFTs as defined above, where the input array X of length N is purely real and is also even. In this case, the output array is likewise real and even.
For the case of REDFT00
, this even symmetry means that
Xj = XN-j,
where we take X to be periodic so that
XN = X0.
Because of this redundancy, only the first n real numbers are
actually stored, where N = 2(n-1).
The proper definition of even symmetry for REDFT10
,
REDFT01
, and REDFT11
transforms is somewhat more intricate
because of the shifts by 1/2 of the input and/or output, although
the corresponding boundary conditions are given in Real even/odd DFTs (cosine/sine transforms). Because of the even symmetry, however,
the sine terms in the DFT all cancel and the remaining cosine terms are
written explicitly below. This formulation often leads people to call
such a transform a discrete cosine transform (DCT), although it is
really just a special case of the DFT.
In each of the definitions below, we transform a real array X of length n to a real array Y of length n:
An REDFT00
transform (type-I DCT) in FFTW is defined by:
An REDFT10
transform (type-II DCT) in FFTW is defined by:
An REDFT01
transform (type-III DCT) in FFTW is defined by:
An REDFT11
transform (type-IV DCT) in FFTW is defined by:
These definitions correspond directly to the unnormalized DFTs used
elsewhere in FFTW (hence the factors of 2 in front of the
summations). The unnormalized inverse of REDFT00
is
REDFT00
, of REDFT10
is REDFT01
and vice versa, and
of REDFT11
is REDFT11
. Each unnormalized inverse results
in the original array multiplied by N, where N is the
logical DFT size. For REDFT00
, N=2(n-1) (note that
n=1 is not defined); otherwise, N=2n.