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I have $FFT(signal)$, and want to find $operation$ such that $$IFFT(operation(FFT(signal),2)) = timestretch(signal, 2)$$

Where $timestretch$ stretches the signal in the time domain - maintaining the frequencies, unlike basic subsampling stretching which leads pitch change.

One option I know I could do is convert to a 2D spectrogram and stretch this "image" and then reverse the spectrogram, but this seems both inaccurate and expensive.

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  • $\begingroup$ Maybe look into the Chirp-Z transform $\endgroup$ – johnnymopo Aug 2 at 18:40
  • $\begingroup$ @johnnymopo this? $\endgroup$ – Tobi Akinyemi Aug 2 at 19:04
  • $\begingroup$ here is how do it in frequency domain phase vocoder $\endgroup$ – ederwander Aug 2 at 21:40
  • $\begingroup$ @ederwander Is the Vocoder technique basically the 2d technique? From what I read it is (they even mention STFT and spectrograms). I don't understand how you do the actually stretching of the spectrogram, they use a pvresample function thats unexplained - and thats the whole meat of the time stretching algorithm (stretching the spectrogram). Is it fine to just do basic stretching of the spectrogram (as if it were an image)? $\endgroup$ – Tobi Akinyemi Aug 2 at 22:21
  • $\begingroup$ in my code there is no pvresample, you must be looking in the wrong place lol, I've never heard of this 2D technique, the phase vocoder is the basis for making time stretch in the frequency domain...all other techniques for doing this in the frequency domain are derived from phase vocoder $\endgroup$ – ederwander Aug 2 at 22:39
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Are you talking about taking an audio recording where someone was speaking too fast, and you want to slow down the speech without changing the pitch? If so, then your original formulation of the problem is incorrect; you can’t do what you want by taking one long FFT of the entire recording and then processIng it. The usual way this is solved is by using the phase vocoder, where you break the signal into overlapping blocks and transform each block. This is a deep subject with lots of tricks to avoid artifacts.

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Your "$\text{timestretch}(\text{signal}, k)$" is what we call "interpolation by $k$", usually. (if you don't believe it: try for yourself!)

Let us adopt a sensible notation (and not call function English words, which typically leads to confusion).

  • $s\in \mathbb C^N$: discrete time input signal of length $N$
  • $m\in\mathbb N$: interpolation ratio
  • $r\in \mathbb C^{mN},\, m\in\mathbb N$: $m$ times as long output signal, subject to:
    • $r[ln] = s[n],\,n\in\mathbb Z,\,l \in \mathbb N$ (i.e. the stretched signal still goes through the same points as the original: "interpolation criterion")
    • $\text{DFT}\{r\}[f] <\epsilon \text{ for } |f| > N/2,\, \epsilon > 0$ (image suppression to at most a small $\epsilon$)

So, there's very many resampling / interpolation algorithms that you could employ.

The probably simplest is zero padding, i.e you take the $\text{DFT}\{r\}$, which is inherently $N$ long, extend the result by $(m-1)N$ zeros, making it $mN$ values long, and do the inverse transform.
That amounts to sinc interpolation due to the convolution theorem of the DFT and the fact that zero-padding mathematically "looks" like you've taken a $N$-periodic signal and multiplied it with an $N$-long rectangular window.

So, your $operation$ is just plain boring "appending zeros until you hit the target length". Often, DSP is that easy!

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  • $\begingroup$ This isn't the time-stretching I was talking about. This is naive stretching using subsampling/interpolation - the pitch isn't preserved like I desired $\endgroup$ – Tobi Akinyemi Aug 3 at 18:31
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Say the FFT array is X[0:N-1]. What you want to do is something like this

for n in range(S * N):
    if mod(n,S) == 0:
        Y[n] = S*X[n/S]
    else:
        Y[n] = 0;
y = ifft(Y)

Effectively you are keeping the radial frequency information the same but scaling the number of samples used by S.

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  • $\begingroup$ What @Bob says in his answer is correct, this solution would need to be performed on time blocks of a signal. There is probably a way of using some gaussian or other window and going along sample by sample of the original signal doing this, but it’s beyond my knowledge. $\endgroup$ – AnalogEE Aug 4 at 20:42

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