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Note that windows applied to the MDCT are different from windows used for some other types of signal analysis, since they must fulfill the Princen–Bradley condition. One of the reasons for this difference is that MDCT windows are applied twice, for both the MDCT (analysis) and the IMDCT (synthesis).
== Relationship to DCT-IV and
As can be seen by inspection of the definitions, for
In order to define the precise relationship to the DCT-IV, one must realize that the DCT-IV corresponds to alternating even/odd boundary conditions: even at its left boundary (around ''n'' = −1/2), odd at its right boundary (around ''n'' = ''N'' − 1/2), and so on (instead of periodic boundaries as for a [[discrete Fourier transform|DFT]]). This follows from the identities
: <math>\cos\left[\frac{\pi}{N} \left(-n - 1 + \frac{1}{2}\right) \left(k + \frac{1}{2}\right)\right] = \cos\left[\frac{\pi}{N} \left(n + \frac{1}{2}\right) \left(k + \frac{1}{2}\right)\right]</math> and : <math>\cos\left[\frac{\pi}{N} \left(2N - n - 1 + \frac{1}{2}\right) \left(k + \frac{1}{2}\right)\right] = -\cos\left[\frac{\pi}{N} \left(n + \frac{1}{2}\right) \left(k + \frac{1}{2}\right)\right].</math> Thus, if its inputs are an array ''x'' of length ''N'', we can imagine extending this array to (''x'', −''x''<sub>''R''</sub>, −''x'', ''x''<sub>''R''</sub>, ...) and so on, where ''x''<sub>''R''</sub> denotes ''x'' in reverse order. Consider an MDCT with 2''N'' inputs and ''N'' outputs, where we divide the inputs into four blocks (''a'', ''b'', ''c'', ''d'') each of size ''N''/2. If we shift these to the right by ''N''/2 (from the +''N''/2 term in the MDCT definition), then (''b'', ''c'', ''d'') extend past the end of the ''N'' DCT-IV inputs, so we must "fold" them back according to the boundary conditions described above.
: Thus, the MDCT of 2''N'' inputs (''a'', ''b'', ''c'', ''d'') is ''exactly'' equivalent to a DCT-IV of the ''N'' inputs: (−''c''<sub>''R''</sub> − ''d'', ''a'' − ''b''<sub>''R''</sub>), where ''R'' denotes reversal as above.
Similarly, the IMDCT formula above is precisely 1/2 of the DCT-IV (which is its own inverse), where the output is extended (via the boundary conditions) to a length 2''N'' and shifted back to the left by ''N''/2. The inverse DCT-IV would simply give back the inputs (−''c''<sub>''R''</sub> − ''d'', ''a'' − ''b''<sub>''R''</sub>) from above. When this is extended via the boundary conditions and shifted, one obtains
: IMDCT(MDCT(''a'', ''b'', ''c'', ''d'')) = (''a'' − ''b''<sub>''R''</sub>, ''b'' − ''a''<sub>''R''</sub>, ''c'' + ''d''<sub>''R''</sub>, ''d'' + ''c''<sub>''R''</sub>)/2.
: IMDCT
One can now understand how TDAC works. Suppose that one computes the MDCT of the subsequent, 50% overlapped, 2''N'' block (''B'', ''C''). The IMDCT will then yield, analogous to the above: (''B'' − ''B''<sub>''R''</sub>, ''C'' + ''C''<sub>''R''</sub>)
▲:IMDCT (MDCT (''A'', ''B'')) = (''A''−''A''<sub>''R''</sub>, ''B''+''B''<sub>''R''</sub>) / 2
▲One can now understand how TDAC works. Suppose that one computes the MDCT of the subsequent, 50% overlapped, 2''N'' block (''B'', ''C''). The IMDCT will then yield, analogous to the above: (''B''−''B''<sub>''R''</sub>, ''C''+''C''<sub>''R''</sub>) / 2. When this is added with the previous IMDCT result in the overlapping half, the reversed terms cancel and one obtains simply ''B'', recovering the original data.
=== Origin of TDAC ===
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