mars.tensor.fft.hfft(a, n=None, axis=-1, norm=None)[source]#

Compute the FFT of a signal that has Hermitian symmetry, i.e., a real spectrum.

  • a (array_like) – The input tensor.

  • n (int, optional) – 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 determined from the length of the input along the axis specified by axis.

  • axis (int, optional) – Axis over which to compute the FFT. If not given, the last axis is used.

  • norm ({None, "ortho"}, optional) – Normalization mode (see mt.fft). Default is None.


out – 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,

Return type



IndexError – If axis is larger than the last axis of a.

See also


Compute the one-dimensional FFT for real input.


The inverse of hfft.


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.


>>> import mars.tensor as mt
>>> signal = mt.array([1, 2, 3, 4, 3, 2])
>>> mt.fft.fft(signal).execute()
array([ 15.+0.j,  -4.+0.j,   0.+0.j,  -1.-0.j,   0.+0.j,  -4.+0.j])
>>> mt.fft.hfft(signal[:4]).execute() # Input first half of signal
array([ 15.,  -4.,   0.,  -1.,   0.,  -4.])
>>> mt.fft.hfft(signal, 6).execute()  # Input entire signal and truncate
array([ 15.,  -4.,   0.,  -1.,   0.,  -4.])
>>> signal = mt.array([[1, 1.j], [-1.j, 2]])
>>> (mt.conj(signal.T) - signal).execute()   # check Hermitian symmetry
array([[ 0.-0.j,  0.+0.j],
       [ 0.+0.j,  0.-0.j]])
>>> freq_spectrum = mt.fft.hfft(signal)
>>> freq_spectrum.execute()
array([[ 1.,  1.],
       [ 2., -2.]])