hfft
/ihfft
are a pair analogous to rfft
/irfft
, but for the opposite case: here, the signal has Hermitian symmetry in the time domain and is real in the frequency domain. So, here, it's hfft
, for which you must supply the length of the result if it is to be odd: * even: ihfft(hfft(a, 2*len(a) - 2) == a
, within roundoff error, * odd: ihfft(hfft(a, 2*len(a) - 1) == a
, within roundoff error.
Input array.
Length of the inverse FFT, the number of points along transformation axis in the input to use. If n
is smaller than the length of the input, the input is cropped. If it is larger, the input is padded with zeros. If n
is not given, the length of the input along the axis specified by :None:None:`axis`
is used.
Axis over which to compute the inverse FFT. If not given, the last axis is used.
Normalization mode (see fft
). Default is "backward".
If True, the contents of x
can be destroyed; the default is False. See fft
for more details.
Maximum number of workers to use for parallel computation. If negative, the value wraps around from os.cpu_count()
. See ~scipy.fft.fft
for more details.
This argument is reserved for passing in a precomputed plan provided by downstream FFT vendors. It is currently not used in SciPy.
The truncated or zero-padded input, transformed along the axis indicated by :None:None:`axis`
, or the last one if :None:None:`axis`
is not specified. The length of the transformed axis is n//2 + 1
.
Compute the inverse FFT of a signal that has Hermitian symmetry.
>>> from scipy.fft import ifft, ihfft
... spectrum = np.array([ 15, -4, 0, -1, 0, -4])
... ifft(spectrum) array([1.+0.j, 2.+0.j, 3.+0.j, 4.+0.j, 3.+0.j, 2.+0.j]) # may vary
>>> ihfft(spectrum) array([ 1.-0.j, 2.-0.j, 3.-0.j, 4.-0.j]) # may varySee :
The following pages refer to to this document either explicitly or contain code examples using this.
scipy.fft._basic.ihfftn
scipy.fft._basic.hfft
scipy.fft._basic.ihfft
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