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scipy.signal.windows.

# general_cosine

scipy.signal.windows.general_cosine(M, a, sym=True)

  Generic weighted sum of cosine terms window

  Parameters:
    M int

      Number of points in the output window

    a array_like

      Sequence of weighting coefficients. This uses the convention of being centered on the origin, so these will typically all be positive numbers, not alternating sign.

    sym bool, optional

      When True (default), generates a symmetric window, for use in filter design. When False, generates a periodic window, for use in spectral analysis.

  Returns:
    w ndarray

      The array of window values.

  Notes

  Array API Standard Support

  `general_cosine` has experimental support for Python Array API Standard compatible backends in addition to NumPy. Please consider testing these features by setting an environment variable `SCIPY_ARRAY_API=1` and providing CuPy, PyTorch, JAX, or Dask arrays as array arguments. The following combinations of backend and device (or other capability) are supported.

  Library | CPU | GPU
  --- | --- | ---
  NumPy | ✅ | n/a
  CuPy | n/a | ✅
  PyTorch | ✅ | ✅
  JAX | ✅ | ✅
  Dask | ✅ | n/a

  > See Support for the array API standard for more information.

  References

  [1]

  A. Nuttall, “Some windows with very good sidelobe behavior,” IEEE Transactions on Acoustics, Speech, and Signal Processing, vol. 29, no. 1, pp. 84-91, Feb 1981. DOI:10.1109/TASSP.1981.1163506.

  [2]

  Heinzel G. et al., “Spectrum and spectral density estimation by the Discrete Fourier transform (DFT), including a comprehensive list of window functions and some new flat-top windows”, February 15, 2002 https://holometer.fnal.gov/GH_FFT.pdf

  Examples

  Heinzel describes a flat-top window named “HFT90D” with formula: [2]

  \[w_j = 1 - 1.942604 \cos(z) + 1.340318 \cos(2z) - 0.440811 \cos(3z) + 0.043097 \cos(4z)\]

  where

  \[z = \frac{2 \pi j}{N}, j = 0...N - 1\]

  Since this uses the convention of starting at the origin, to reproduce the window, we need to convert every other coefficient to a positive number:

      >>> HFT90D = [1, 1.942604, 1.340318, 0.440811, 0.043097]

  The paper states that the highest sidelobe is at -90.2 dB. Reproduce Figure 42 by plotting the window and its frequency response, and confirm the sidelobe level in red:

      >>> import numpy as np
      >>> from scipy.signal.windows import general_cosine
      >>> from scipy.fft import fft, fftshift
      >>> import matplotlib.pyplot as plt

      >>> window = general_cosine(1000, HFT90D, sym=False)
      >>> plt.plot(window)
      >>> plt.title("HFT90D window")
      >>> plt.ylabel("Amplitude")
      >>> plt.xlabel("Sample")

      >>> plt.figure()
      >>> A = fft(window, 10000) / (len(window)/2.0)
      >>> freq = np.linspace(-0.5, 0.5, len(A))
      >>> response = np.abs(fftshift(A / abs(A).max()))
      >>> response = 20 * np.log10(np.maximum(response, 1e-10))
      >>> plt.plot(freq, response)
      >>> plt.axis([-50/1000, 50/1000, -140, 0])
      >>> plt.title("Frequency response of the HFT90D window")
      >>> plt.ylabel("Normalized magnitude [dB]")
      >>> plt.xlabel("Normalized frequency [cycles per sample]")
      >>> plt.axhline(-90.2, color='red')
      >>> plt.show()