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Compute the FFT of a signal that has Hermitian symmetry, i.e., a real spectrum.
The input array.
Length of the transformed axis of the output. For n output
points, n//2 + 1 input points are necessary. If the input is
longer than this, it is cropped. If it is shorter than this, it is
padded with zeros. If n is not given, it is taken to be 2*(m-1)
where m is the length of the input along the axis specified by
axis.
Axis over which to compute the FFT. If not given, the last axis is used.
Normalization mode (see numpy.fft). Default is backward.
Indicates which direction of the forward/backward pair of transforms
is scaled and with what normalization factor.
New in version 1.20.0: The backward, forward values were added.
If provided, the result will be placed in this array. It should be of the appropriate shape and dtype.
New in version 2.0.0.
The truncated or zero-padded input, transformed along the axis
indicated by axis, or the last one if axis is not specified.
The length of the transformed axis is n, or, if n is not given,
2*m - 2 where m is the length of the transformed axis of
the input. To get an odd number of output points, n must be
specified, for instance as 2*m - 1 in the typical case,
If axis is not a valid axis of a.
Notes
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 its 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.
The correct interpretation of the hermitian input depends on the length of
the original data, as given by n. This is because each input shape could
correspond to either an odd or even length signal. By default, hfft
assumes an even output length which puts the last entry at the Nyquist
frequency; aliasing with its symmetric counterpart. By Hermitian symmetry,
the value is thus treated as purely real. To avoid losing information, the
shape of the full signal must be given.
Examples
>>> import numpy as np
>>> signal = np.array([1, 2, 3, 4, 3, 2])
>>> np.fft.fft(signal)
array([15.+0.j, -4.+0.j, 0.+0.j, -1.-0.j, 0.+0.j, -4.+0.j]) # may vary
>>> np.fft.hfft(signal[:4]) # Input first half of signal
array([15., -4., 0., -1., 0., -4.])
>>> np.fft.hfft(signal, 6) # Input entire signal and truncate
array([15., -4., 0., -1., 0., -4.])
>>> signal = np.array([[1, 1.j], [-1.j, 2]])
>>> np.conj(signal.T) - signal # check Hermitian symmetry
array([[ 0.-0.j, -0.+0.j], # may vary
[ 0.+0.j, 0.-0.j]])
>>> freq_spectrum = np.fft.hfft(signal)
>>> freq_spectrum
array([[ 1., 1.],
[ 2., -2.]])
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