peacock-data-public-datasets-idc-llm_eval
/
env-llmeval
/lib
/python3.10
/site-packages
/numpy
/fft
/_pocketfft.py
| """ | |
| Discrete Fourier Transforms | |
| Routines in this module: | |
| fft(a, n=None, axis=-1, norm="backward") | |
| ifft(a, n=None, axis=-1, norm="backward") | |
| rfft(a, n=None, axis=-1, norm="backward") | |
| irfft(a, n=None, axis=-1, norm="backward") | |
| hfft(a, n=None, axis=-1, norm="backward") | |
| ihfft(a, n=None, axis=-1, norm="backward") | |
| fftn(a, s=None, axes=None, norm="backward") | |
| ifftn(a, s=None, axes=None, norm="backward") | |
| rfftn(a, s=None, axes=None, norm="backward") | |
| irfftn(a, s=None, axes=None, norm="backward") | |
| fft2(a, s=None, axes=(-2,-1), norm="backward") | |
| ifft2(a, s=None, axes=(-2, -1), norm="backward") | |
| rfft2(a, s=None, axes=(-2,-1), norm="backward") | |
| irfft2(a, s=None, axes=(-2, -1), norm="backward") | |
| i = inverse transform | |
| r = transform of purely real data | |
| h = Hermite transform | |
| n = n-dimensional transform | |
| 2 = 2-dimensional transform | |
| (Note: 2D routines are just nD routines with different default | |
| behavior.) | |
| """ | |
| __all__ = ['fft', 'ifft', 'rfft', 'irfft', 'hfft', 'ihfft', 'rfftn', | |
| 'irfftn', 'rfft2', 'irfft2', 'fft2', 'ifft2', 'fftn', 'ifftn'] | |
| import functools | |
| from numpy.core import asarray, zeros, swapaxes, conjugate, take, sqrt | |
| from . import _pocketfft_internal as pfi | |
| from numpy.core.multiarray import normalize_axis_index | |
| from numpy.core import overrides | |
| array_function_dispatch = functools.partial( | |
| overrides.array_function_dispatch, module='numpy.fft') | |
| # `inv_norm` is a float by which the result of the transform needs to be | |
| # divided. This replaces the original, more intuitive 'fct` parameter to avoid | |
| # divisions by zero (or alternatively additional checks) in the case of | |
| # zero-length axes during its computation. | |
| def _raw_fft(a, n, axis, is_real, is_forward, inv_norm): | |
| axis = normalize_axis_index(axis, a.ndim) | |
| if n is None: | |
| n = a.shape[axis] | |
| fct = 1/inv_norm | |
| if a.shape[axis] != n: | |
| s = list(a.shape) | |
| index = [slice(None)]*len(s) | |
| if s[axis] > n: | |
| index[axis] = slice(0, n) | |
| a = a[tuple(index)] | |
| else: | |
| index[axis] = slice(0, s[axis]) | |
| s[axis] = n | |
| z = zeros(s, a.dtype.char) | |
| z[tuple(index)] = a | |
| a = z | |
| if axis == a.ndim-1: | |
| r = pfi.execute(a, is_real, is_forward, fct) | |
| else: | |
| a = swapaxes(a, axis, -1) | |
| r = pfi.execute(a, is_real, is_forward, fct) | |
| r = swapaxes(r, axis, -1) | |
| return r | |
| def _get_forward_norm(n, norm): | |
| if n < 1: | |
| raise ValueError(f"Invalid number of FFT data points ({n}) specified.") | |
| if norm is None or norm == "backward": | |
| return 1 | |
| elif norm == "ortho": | |
| return sqrt(n) | |
| elif norm == "forward": | |
| return n | |
| raise ValueError(f'Invalid norm value {norm}; should be "backward",' | |
| '"ortho" or "forward".') | |
| def _get_backward_norm(n, norm): | |
| if n < 1: | |
| raise ValueError(f"Invalid number of FFT data points ({n}) specified.") | |
| if norm is None or norm == "backward": | |
| return n | |
| elif norm == "ortho": | |
| return sqrt(n) | |
| elif norm == "forward": | |
| return 1 | |
| raise ValueError(f'Invalid norm value {norm}; should be "backward", ' | |
| '"ortho" or "forward".') | |
| _SWAP_DIRECTION_MAP = {"backward": "forward", None: "forward", | |
| "ortho": "ortho", "forward": "backward"} | |
| def _swap_direction(norm): | |
| try: | |
| return _SWAP_DIRECTION_MAP[norm] | |
| except KeyError: | |
| raise ValueError(f'Invalid norm value {norm}; should be "backward", ' | |
| '"ortho" or "forward".') from None | |
| def _fft_dispatcher(a, n=None, axis=None, norm=None): | |
| return (a,) | |
| def fft(a, n=None, axis=-1, norm=None): | |
| """ | |
| Compute the one-dimensional discrete Fourier Transform. | |
| This function computes the one-dimensional *n*-point discrete Fourier | |
| Transform (DFT) with the efficient Fast Fourier Transform (FFT) | |
| algorithm [CT]. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array, can be complex. | |
| n : int, optional | |
| Length of the transformed axis of the output. | |
| 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 `axis` is used. | |
| axis : int, optional | |
| Axis over which to compute the FFT. If not given, the last axis is | |
| used. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axis | |
| indicated by `axis`, or the last one if `axis` is not specified. | |
| Raises | |
| ------ | |
| IndexError | |
| If `axis` is not a valid axis of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : for definition of the DFT and conventions used. | |
| ifft : The inverse of `fft`. | |
| fft2 : The two-dimensional FFT. | |
| fftn : The *n*-dimensional FFT. | |
| rfftn : The *n*-dimensional FFT of real input. | |
| fftfreq : Frequency bins for given FFT parameters. | |
| Notes | |
| ----- | |
| FFT (Fast Fourier Transform) refers to a way the discrete Fourier | |
| Transform (DFT) can be calculated efficiently, by using symmetries in the | |
| calculated terms. The symmetry is highest when `n` is a power of 2, and | |
| the transform is therefore most efficient for these sizes. | |
| The DFT is defined, with the conventions used in this implementation, in | |
| the documentation for the `numpy.fft` module. | |
| References | |
| ---------- | |
| .. [CT] Cooley, James W., and John W. Tukey, 1965, "An algorithm for the | |
| machine calculation of complex Fourier series," *Math. Comput.* | |
| 19: 297-301. | |
| Examples | |
| -------- | |
| >>> np.fft.fft(np.exp(2j * np.pi * np.arange(8) / 8)) | |
| array([-2.33486982e-16+1.14423775e-17j, 8.00000000e+00-1.25557246e-15j, | |
| 2.33486982e-16+2.33486982e-16j, 0.00000000e+00+1.22464680e-16j, | |
| -1.14423775e-17+2.33486982e-16j, 0.00000000e+00+5.20784380e-16j, | |
| 1.14423775e-17+1.14423775e-17j, 0.00000000e+00+1.22464680e-16j]) | |
| In this example, real input has an FFT which is Hermitian, i.e., symmetric | |
| in the real part and anti-symmetric in the imaginary part, as described in | |
| the `numpy.fft` documentation: | |
| >>> import matplotlib.pyplot as plt | |
| >>> t = np.arange(256) | |
| >>> sp = np.fft.fft(np.sin(t)) | |
| >>> freq = np.fft.fftfreq(t.shape[-1]) | |
| >>> plt.plot(freq, sp.real, freq, sp.imag) | |
| [<matplotlib.lines.Line2D object at 0x...>, <matplotlib.lines.Line2D object at 0x...>] | |
| >>> plt.show() | |
| """ | |
| a = asarray(a) | |
| if n is None: | |
| n = a.shape[axis] | |
| inv_norm = _get_forward_norm(n, norm) | |
| output = _raw_fft(a, n, axis, False, True, inv_norm) | |
| return output | |
| def ifft(a, n=None, axis=-1, norm=None): | |
| """ | |
| Compute the one-dimensional inverse discrete Fourier Transform. | |
| This function computes the inverse of the one-dimensional *n*-point | |
| discrete Fourier transform computed by `fft`. In other words, | |
| ``ifft(fft(a)) == a`` to within numerical accuracy. | |
| For a general description of the algorithm and definitions, | |
| see `numpy.fft`. | |
| The input should be ordered in the same way as is returned by `fft`, | |
| i.e., | |
| * ``a[0]`` should contain the zero frequency term, | |
| * ``a[1:n//2]`` should contain the positive-frequency terms, | |
| * ``a[n//2 + 1:]`` should contain the negative-frequency terms, in | |
| increasing order starting from the most negative frequency. | |
| For an even number of input points, ``A[n//2]`` represents the sum of | |
| the values at the positive and negative Nyquist frequencies, as the two | |
| are aliased together. See `numpy.fft` for details. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array, can be complex. | |
| n : int, optional | |
| Length of the transformed axis of the output. | |
| 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 `axis` is used. | |
| See notes about padding issues. | |
| axis : int, optional | |
| Axis over which to compute the inverse DFT. If not given, the last | |
| axis is used. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axis | |
| indicated by `axis`, or the last one if `axis` is not specified. | |
| Raises | |
| ------ | |
| IndexError | |
| If `axis` is not a valid axis of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : An introduction, with definitions and general explanations. | |
| fft : The one-dimensional (forward) FFT, of which `ifft` is the inverse | |
| ifft2 : The two-dimensional inverse FFT. | |
| ifftn : The n-dimensional inverse FFT. | |
| Notes | |
| ----- | |
| If the input parameter `n` is larger than the size of the input, the input | |
| is padded by appending zeros at the end. Even though this is the common | |
| approach, it might lead to surprising results. If a different padding is | |
| desired, it must be performed before calling `ifft`. | |
| Examples | |
| -------- | |
| >>> np.fft.ifft([0, 4, 0, 0]) | |
| array([ 1.+0.j, 0.+1.j, -1.+0.j, 0.-1.j]) # may vary | |
| Create and plot a band-limited signal with random phases: | |
| >>> import matplotlib.pyplot as plt | |
| >>> t = np.arange(400) | |
| >>> n = np.zeros((400,), dtype=complex) | |
| >>> n[40:60] = np.exp(1j*np.random.uniform(0, 2*np.pi, (20,))) | |
| >>> s = np.fft.ifft(n) | |
| >>> plt.plot(t, s.real, label='real') | |
| [<matplotlib.lines.Line2D object at ...>] | |
| >>> plt.plot(t, s.imag, '--', label='imaginary') | |
| [<matplotlib.lines.Line2D object at ...>] | |
| >>> plt.legend() | |
| <matplotlib.legend.Legend object at ...> | |
| >>> plt.show() | |
| """ | |
| a = asarray(a) | |
| if n is None: | |
| n = a.shape[axis] | |
| inv_norm = _get_backward_norm(n, norm) | |
| output = _raw_fft(a, n, axis, False, False, inv_norm) | |
| return output | |
| def rfft(a, n=None, axis=-1, norm=None): | |
| """ | |
| Compute the one-dimensional discrete Fourier Transform for real input. | |
| This function computes the one-dimensional *n*-point discrete Fourier | |
| Transform (DFT) of a real-valued array by means of an efficient algorithm | |
| called the Fast Fourier Transform (FFT). | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array | |
| n : int, optional | |
| 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 `axis` is used. | |
| axis : int, optional | |
| Axis over which to compute the FFT. If not given, the last axis is | |
| used. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axis | |
| indicated by `axis`, or the last one if `axis` is not specified. | |
| If `n` is even, the length of the transformed axis is ``(n/2)+1``. | |
| If `n` is odd, the length is ``(n+1)/2``. | |
| Raises | |
| ------ | |
| IndexError | |
| If `axis` is not a valid axis of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : For definition of the DFT and conventions used. | |
| irfft : The inverse of `rfft`. | |
| fft : The one-dimensional FFT of general (complex) input. | |
| fftn : The *n*-dimensional FFT. | |
| rfftn : The *n*-dimensional FFT of real input. | |
| Notes | |
| ----- | |
| When the DFT is computed for purely real input, the output is | |
| Hermitian-symmetric, i.e. the negative frequency terms are just the complex | |
| conjugates of the corresponding positive-frequency terms, and the | |
| negative-frequency terms are therefore redundant. This function does not | |
| compute the negative frequency terms, and the length of the transformed | |
| axis of the output is therefore ``n//2 + 1``. | |
| When ``A = rfft(a)`` and fs is the sampling frequency, ``A[0]`` contains | |
| the zero-frequency term 0*fs, which is real due to Hermitian symmetry. | |
| If `n` is even, ``A[-1]`` contains the term representing both positive | |
| and negative Nyquist frequency (+fs/2 and -fs/2), and must also be purely | |
| real. If `n` is odd, there is no term at fs/2; ``A[-1]`` contains | |
| the largest positive frequency (fs/2*(n-1)/n), and is complex in the | |
| general case. | |
| If the input `a` contains an imaginary part, it is silently discarded. | |
| Examples | |
| -------- | |
| >>> np.fft.fft([0, 1, 0, 0]) | |
| array([ 1.+0.j, 0.-1.j, -1.+0.j, 0.+1.j]) # may vary | |
| >>> np.fft.rfft([0, 1, 0, 0]) | |
| array([ 1.+0.j, 0.-1.j, -1.+0.j]) # may vary | |
| Notice how the final element of the `fft` output is the complex conjugate | |
| of the second element, for real input. For `rfft`, this symmetry is | |
| exploited to compute only the non-negative frequency terms. | |
| """ | |
| a = asarray(a) | |
| if n is None: | |
| n = a.shape[axis] | |
| inv_norm = _get_forward_norm(n, norm) | |
| output = _raw_fft(a, n, axis, True, True, inv_norm) | |
| return output | |
| def irfft(a, n=None, axis=-1, norm=None): | |
| """ | |
| Computes the inverse of `rfft`. | |
| This function computes the inverse of the one-dimensional *n*-point | |
| discrete Fourier Transform of real input computed by `rfft`. | |
| In other words, ``irfft(rfft(a), len(a)) == a`` to within numerical | |
| accuracy. (See Notes below for why ``len(a)`` is necessary here.) | |
| The input is expected to be in the form returned by `rfft`, i.e. the | |
| real zero-frequency term followed by the complex positive frequency terms | |
| in order of increasing frequency. Since the discrete Fourier Transform of | |
| real input is Hermitian-symmetric, the negative frequency terms are taken | |
| to be the complex conjugates of the corresponding positive frequency terms. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| The input array. | |
| 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 taken to be | |
| ``2*(m-1)`` where ``m`` is the length of the input along the axis | |
| specified by `axis`. | |
| axis : int, optional | |
| Axis over which to compute the inverse FFT. If not given, the last | |
| axis is used. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : ndarray | |
| 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-1)`` where ``m`` is the length of the transformed axis of the | |
| input. To get an odd number of output points, `n` must be specified. | |
| Raises | |
| ------ | |
| IndexError | |
| If `axis` is not a valid axis of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : For definition of the DFT and conventions used. | |
| rfft : The one-dimensional FFT of real input, of which `irfft` is inverse. | |
| fft : The one-dimensional FFT. | |
| irfft2 : The inverse of the two-dimensional FFT of real input. | |
| irfftn : The inverse of the *n*-dimensional FFT of real input. | |
| Notes | |
| ----- | |
| Returns the real valued `n`-point inverse discrete Fourier transform | |
| of `a`, where `a` contains the non-negative frequency terms of a | |
| Hermitian-symmetric sequence. `n` is the length of the result, not the | |
| input. | |
| If you specify an `n` such that `a` must be zero-padded or truncated, the | |
| extra/removed values will be added/removed at high frequencies. One can | |
| thus resample a series to `m` points via Fourier interpolation by: | |
| ``a_resamp = irfft(rfft(a), m)``. | |
| 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, `irfft` | |
| 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 | |
| correct length of the real input **must** be given. | |
| Examples | |
| -------- | |
| >>> np.fft.ifft([1, -1j, -1, 1j]) | |
| array([0.+0.j, 1.+0.j, 0.+0.j, 0.+0.j]) # may vary | |
| >>> np.fft.irfft([1, -1j, -1]) | |
| array([0., 1., 0., 0.]) | |
| Notice how the last term in the input to the ordinary `ifft` is the | |
| complex conjugate of the second term, and the output has zero imaginary | |
| part everywhere. When calling `irfft`, the negative frequencies are not | |
| specified, and the output array is purely real. | |
| """ | |
| a = asarray(a) | |
| if n is None: | |
| n = (a.shape[axis] - 1) * 2 | |
| inv_norm = _get_backward_norm(n, norm) | |
| output = _raw_fft(a, n, axis, True, False, inv_norm) | |
| return output | |
| def hfft(a, n=None, axis=-1, norm=None): | |
| """ | |
| Compute the FFT of a signal that has Hermitian symmetry, i.e., a real | |
| spectrum. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| The input array. | |
| 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 taken to be ``2*(m-1)`` | |
| where ``m`` is 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 : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : ndarray | |
| 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, | |
| Raises | |
| ------ | |
| IndexError | |
| If `axis` is not a valid axis of `a`. | |
| See also | |
| -------- | |
| rfft : Compute the one-dimensional FFT for real input. | |
| ihfft : The inverse of `hfft`. | |
| 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 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. | |
| 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 | |
| -------- | |
| >>> 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.]]) | |
| """ | |
| a = asarray(a) | |
| if n is None: | |
| n = (a.shape[axis] - 1) * 2 | |
| new_norm = _swap_direction(norm) | |
| output = irfft(conjugate(a), n, axis, norm=new_norm) | |
| return output | |
| def ihfft(a, n=None, axis=-1, norm=None): | |
| """ | |
| Compute the inverse FFT of a signal that has Hermitian symmetry. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array. | |
| n : int, optional | |
| 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 `axis` is used. | |
| axis : int, optional | |
| Axis over which to compute the inverse FFT. If not given, the last | |
| axis is used. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| 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//2 + 1``. | |
| See also | |
| -------- | |
| hfft, irfft | |
| 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 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. | |
| Examples | |
| -------- | |
| >>> spectrum = np.array([ 15, -4, 0, -1, 0, -4]) | |
| >>> np.fft.ifft(spectrum) | |
| array([1.+0.j, 2.+0.j, 3.+0.j, 4.+0.j, 3.+0.j, 2.+0.j]) # may vary | |
| >>> np.fft.ihfft(spectrum) | |
| array([ 1.-0.j, 2.-0.j, 3.-0.j, 4.-0.j]) # may vary | |
| """ | |
| a = asarray(a) | |
| if n is None: | |
| n = a.shape[axis] | |
| new_norm = _swap_direction(norm) | |
| output = conjugate(rfft(a, n, axis, norm=new_norm)) | |
| return output | |
| def _cook_nd_args(a, s=None, axes=None, invreal=0): | |
| if s is None: | |
| shapeless = 1 | |
| if axes is None: | |
| s = list(a.shape) | |
| else: | |
| s = take(a.shape, axes) | |
| else: | |
| shapeless = 0 | |
| s = list(s) | |
| if axes is None: | |
| axes = list(range(-len(s), 0)) | |
| if len(s) != len(axes): | |
| raise ValueError("Shape and axes have different lengths.") | |
| if invreal and shapeless: | |
| s[-1] = (a.shape[axes[-1]] - 1) * 2 | |
| return s, axes | |
| def _raw_fftnd(a, s=None, axes=None, function=fft, norm=None): | |
| a = asarray(a) | |
| s, axes = _cook_nd_args(a, s, axes) | |
| itl = list(range(len(axes))) | |
| itl.reverse() | |
| for ii in itl: | |
| a = function(a, n=s[ii], axis=axes[ii], norm=norm) | |
| return a | |
| def _fftn_dispatcher(a, s=None, axes=None, norm=None): | |
| return (a,) | |
| def fftn(a, s=None, axes=None, norm=None): | |
| """ | |
| Compute the N-dimensional discrete Fourier Transform. | |
| This function computes the *N*-dimensional discrete Fourier Transform over | |
| any number of axes in an *M*-dimensional array by means of the Fast Fourier | |
| Transform (FFT). | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array, can be complex. | |
| s : sequence of ints, optional | |
| Shape (length of each transformed axis) of the output | |
| (``s[0]`` refers to axis 0, ``s[1]`` to axis 1, etc.). | |
| This corresponds to ``n`` for ``fft(x, n)``. | |
| Along any axis, if the given shape is smaller than that of the input, | |
| the input is cropped. If it is larger, the input is padded with zeros. | |
| if `s` is not given, the shape of the input along the axes specified | |
| by `axes` is used. | |
| axes : sequence of ints, optional | |
| Axes over which to compute the FFT. If not given, the last ``len(s)`` | |
| axes are used, or all axes if `s` is also not specified. | |
| Repeated indices in `axes` means that the transform over that axis is | |
| performed multiple times. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axes | |
| indicated by `axes`, or by a combination of `s` and `a`, | |
| as explained in the parameters section above. | |
| Raises | |
| ------ | |
| ValueError | |
| If `s` and `axes` have different length. | |
| IndexError | |
| If an element of `axes` is larger than than the number of axes of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : Overall view of discrete Fourier transforms, with definitions | |
| and conventions used. | |
| ifftn : The inverse of `fftn`, the inverse *n*-dimensional FFT. | |
| fft : The one-dimensional FFT, with definitions and conventions used. | |
| rfftn : The *n*-dimensional FFT of real input. | |
| fft2 : The two-dimensional FFT. | |
| fftshift : Shifts zero-frequency terms to centre of array | |
| Notes | |
| ----- | |
| The output, analogously to `fft`, contains the term for zero frequency in | |
| the low-order corner of all axes, the positive frequency terms in the | |
| first half of all axes, the term for the Nyquist frequency in the middle | |
| of all axes and the negative frequency terms in the second half of all | |
| axes, in order of decreasingly negative frequency. | |
| See `numpy.fft` for details, definitions and conventions used. | |
| Examples | |
| -------- | |
| >>> a = np.mgrid[:3, :3, :3][0] | |
| >>> np.fft.fftn(a, axes=(1, 2)) | |
| array([[[ 0.+0.j, 0.+0.j, 0.+0.j], # may vary | |
| [ 0.+0.j, 0.+0.j, 0.+0.j], | |
| [ 0.+0.j, 0.+0.j, 0.+0.j]], | |
| [[ 9.+0.j, 0.+0.j, 0.+0.j], | |
| [ 0.+0.j, 0.+0.j, 0.+0.j], | |
| [ 0.+0.j, 0.+0.j, 0.+0.j]], | |
| [[18.+0.j, 0.+0.j, 0.+0.j], | |
| [ 0.+0.j, 0.+0.j, 0.+0.j], | |
| [ 0.+0.j, 0.+0.j, 0.+0.j]]]) | |
| >>> np.fft.fftn(a, (2, 2), axes=(0, 1)) | |
| array([[[ 2.+0.j, 2.+0.j, 2.+0.j], # may vary | |
| [ 0.+0.j, 0.+0.j, 0.+0.j]], | |
| [[-2.+0.j, -2.+0.j, -2.+0.j], | |
| [ 0.+0.j, 0.+0.j, 0.+0.j]]]) | |
| >>> import matplotlib.pyplot as plt | |
| >>> [X, Y] = np.meshgrid(2 * np.pi * np.arange(200) / 12, | |
| ... 2 * np.pi * np.arange(200) / 34) | |
| >>> S = np.sin(X) + np.cos(Y) + np.random.uniform(0, 1, X.shape) | |
| >>> FS = np.fft.fftn(S) | |
| >>> plt.imshow(np.log(np.abs(np.fft.fftshift(FS))**2)) | |
| <matplotlib.image.AxesImage object at 0x...> | |
| >>> plt.show() | |
| """ | |
| return _raw_fftnd(a, s, axes, fft, norm) | |
| def ifftn(a, s=None, axes=None, norm=None): | |
| """ | |
| Compute the N-dimensional inverse discrete Fourier Transform. | |
| This function computes the inverse of the N-dimensional discrete | |
| Fourier Transform over any number of axes in an M-dimensional array by | |
| means of the Fast Fourier Transform (FFT). In other words, | |
| ``ifftn(fftn(a)) == a`` to within numerical accuracy. | |
| For a description of the definitions and conventions used, see `numpy.fft`. | |
| The input, analogously to `ifft`, should be ordered in the same way as is | |
| returned by `fftn`, i.e. it should have the term for zero frequency | |
| in all axes in the low-order corner, the positive frequency terms in the | |
| first half of all axes, the term for the Nyquist frequency in the middle | |
| of all axes and the negative frequency terms in the second half of all | |
| axes, in order of decreasingly negative frequency. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array, can be complex. | |
| s : sequence of ints, optional | |
| Shape (length of each transformed axis) of the output | |
| (``s[0]`` refers to axis 0, ``s[1]`` to axis 1, etc.). | |
| This corresponds to ``n`` for ``ifft(x, n)``. | |
| Along any axis, if the given shape is smaller than that of the input, | |
| the input is cropped. If it is larger, the input is padded with zeros. | |
| if `s` is not given, the shape of the input along the axes specified | |
| by `axes` is used. See notes for issue on `ifft` zero padding. | |
| axes : sequence of ints, optional | |
| Axes over which to compute the IFFT. If not given, the last ``len(s)`` | |
| axes are used, or all axes if `s` is also not specified. | |
| Repeated indices in `axes` means that the inverse transform over that | |
| axis is performed multiple times. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axes | |
| indicated by `axes`, or by a combination of `s` or `a`, | |
| as explained in the parameters section above. | |
| Raises | |
| ------ | |
| ValueError | |
| If `s` and `axes` have different length. | |
| IndexError | |
| If an element of `axes` is larger than than the number of axes of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : Overall view of discrete Fourier transforms, with definitions | |
| and conventions used. | |
| fftn : The forward *n*-dimensional FFT, of which `ifftn` is the inverse. | |
| ifft : The one-dimensional inverse FFT. | |
| ifft2 : The two-dimensional inverse FFT. | |
| ifftshift : Undoes `fftshift`, shifts zero-frequency terms to beginning | |
| of array. | |
| Notes | |
| ----- | |
| See `numpy.fft` for definitions and conventions used. | |
| Zero-padding, analogously with `ifft`, is performed by appending zeros to | |
| the input along the specified dimension. Although this is the common | |
| approach, it might lead to surprising results. If another form of zero | |
| padding is desired, it must be performed before `ifftn` is called. | |
| Examples | |
| -------- | |
| >>> a = np.eye(4) | |
| >>> np.fft.ifftn(np.fft.fftn(a, axes=(0,)), axes=(1,)) | |
| array([[1.+0.j, 0.+0.j, 0.+0.j, 0.+0.j], # may vary | |
| [0.+0.j, 1.+0.j, 0.+0.j, 0.+0.j], | |
| [0.+0.j, 0.+0.j, 1.+0.j, 0.+0.j], | |
| [0.+0.j, 0.+0.j, 0.+0.j, 1.+0.j]]) | |
| Create and plot an image with band-limited frequency content: | |
| >>> import matplotlib.pyplot as plt | |
| >>> n = np.zeros((200,200), dtype=complex) | |
| >>> n[60:80, 20:40] = np.exp(1j*np.random.uniform(0, 2*np.pi, (20, 20))) | |
| >>> im = np.fft.ifftn(n).real | |
| >>> plt.imshow(im) | |
| <matplotlib.image.AxesImage object at 0x...> | |
| >>> plt.show() | |
| """ | |
| return _raw_fftnd(a, s, axes, ifft, norm) | |
| def fft2(a, s=None, axes=(-2, -1), norm=None): | |
| """ | |
| Compute the 2-dimensional discrete Fourier Transform. | |
| This function computes the *n*-dimensional discrete Fourier Transform | |
| over any axes in an *M*-dimensional array by means of the | |
| Fast Fourier Transform (FFT). By default, the transform is computed over | |
| the last two axes of the input array, i.e., a 2-dimensional FFT. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array, can be complex | |
| s : sequence of ints, optional | |
| Shape (length of each transformed axis) of the output | |
| (``s[0]`` refers to axis 0, ``s[1]`` to axis 1, etc.). | |
| This corresponds to ``n`` for ``fft(x, n)``. | |
| Along each axis, if the given shape is smaller than that of the input, | |
| the input is cropped. If it is larger, the input is padded with zeros. | |
| if `s` is not given, the shape of the input along the axes specified | |
| by `axes` is used. | |
| axes : sequence of ints, optional | |
| Axes over which to compute the FFT. If not given, the last two | |
| axes are used. A repeated index in `axes` means the transform over | |
| that axis is performed multiple times. A one-element sequence means | |
| that a one-dimensional FFT is performed. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axes | |
| indicated by `axes`, or the last two axes if `axes` is not given. | |
| Raises | |
| ------ | |
| ValueError | |
| If `s` and `axes` have different length, or `axes` not given and | |
| ``len(s) != 2``. | |
| IndexError | |
| If an element of `axes` is larger than than the number of axes of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : Overall view of discrete Fourier transforms, with definitions | |
| and conventions used. | |
| ifft2 : The inverse two-dimensional FFT. | |
| fft : The one-dimensional FFT. | |
| fftn : The *n*-dimensional FFT. | |
| fftshift : Shifts zero-frequency terms to the center of the array. | |
| For two-dimensional input, swaps first and third quadrants, and second | |
| and fourth quadrants. | |
| Notes | |
| ----- | |
| `fft2` is just `fftn` with a different default for `axes`. | |
| The output, analogously to `fft`, contains the term for zero frequency in | |
| the low-order corner of the transformed axes, the positive frequency terms | |
| in the first half of these axes, the term for the Nyquist frequency in the | |
| middle of the axes and the negative frequency terms in the second half of | |
| the axes, in order of decreasingly negative frequency. | |
| See `fftn` for details and a plotting example, and `numpy.fft` for | |
| definitions and conventions used. | |
| Examples | |
| -------- | |
| >>> a = np.mgrid[:5, :5][0] | |
| >>> np.fft.fft2(a) | |
| array([[ 50. +0.j , 0. +0.j , 0. +0.j , # may vary | |
| 0. +0.j , 0. +0.j ], | |
| [-12.5+17.20477401j, 0. +0.j , 0. +0.j , | |
| 0. +0.j , 0. +0.j ], | |
| [-12.5 +4.0614962j , 0. +0.j , 0. +0.j , | |
| 0. +0.j , 0. +0.j ], | |
| [-12.5 -4.0614962j , 0. +0.j , 0. +0.j , | |
| 0. +0.j , 0. +0.j ], | |
| [-12.5-17.20477401j, 0. +0.j , 0. +0.j , | |
| 0. +0.j , 0. +0.j ]]) | |
| """ | |
| return _raw_fftnd(a, s, axes, fft, norm) | |
| def ifft2(a, s=None, axes=(-2, -1), norm=None): | |
| """ | |
| Compute the 2-dimensional inverse discrete Fourier Transform. | |
| This function computes the inverse of the 2-dimensional discrete Fourier | |
| Transform over any number of axes in an M-dimensional array by means of | |
| the Fast Fourier Transform (FFT). In other words, ``ifft2(fft2(a)) == a`` | |
| to within numerical accuracy. By default, the inverse transform is | |
| computed over the last two axes of the input array. | |
| The input, analogously to `ifft`, should be ordered in the same way as is | |
| returned by `fft2`, i.e. it should have the term for zero frequency | |
| in the low-order corner of the two axes, the positive frequency terms in | |
| the first half of these axes, the term for the Nyquist frequency in the | |
| middle of the axes and the negative frequency terms in the second half of | |
| both axes, in order of decreasingly negative frequency. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array, can be complex. | |
| s : sequence of ints, optional | |
| Shape (length of each axis) of the output (``s[0]`` refers to axis 0, | |
| ``s[1]`` to axis 1, etc.). This corresponds to `n` for ``ifft(x, n)``. | |
| Along each axis, if the given shape is smaller than that of the input, | |
| the input is cropped. If it is larger, the input is padded with zeros. | |
| if `s` is not given, the shape of the input along the axes specified | |
| by `axes` is used. See notes for issue on `ifft` zero padding. | |
| axes : sequence of ints, optional | |
| Axes over which to compute the FFT. If not given, the last two | |
| axes are used. A repeated index in `axes` means the transform over | |
| that axis is performed multiple times. A one-element sequence means | |
| that a one-dimensional FFT is performed. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axes | |
| indicated by `axes`, or the last two axes if `axes` is not given. | |
| Raises | |
| ------ | |
| ValueError | |
| If `s` and `axes` have different length, or `axes` not given and | |
| ``len(s) != 2``. | |
| IndexError | |
| If an element of `axes` is larger than than the number of axes of `a`. | |
| See Also | |
| -------- | |
| numpy.fft : Overall view of discrete Fourier transforms, with definitions | |
| and conventions used. | |
| fft2 : The forward 2-dimensional FFT, of which `ifft2` is the inverse. | |
| ifftn : The inverse of the *n*-dimensional FFT. | |
| fft : The one-dimensional FFT. | |
| ifft : The one-dimensional inverse FFT. | |
| Notes | |
| ----- | |
| `ifft2` is just `ifftn` with a different default for `axes`. | |
| See `ifftn` for details and a plotting example, and `numpy.fft` for | |
| definition and conventions used. | |
| Zero-padding, analogously with `ifft`, is performed by appending zeros to | |
| the input along the specified dimension. Although this is the common | |
| approach, it might lead to surprising results. If another form of zero | |
| padding is desired, it must be performed before `ifft2` is called. | |
| Examples | |
| -------- | |
| >>> a = 4 * np.eye(4) | |
| >>> np.fft.ifft2(a) | |
| array([[1.+0.j, 0.+0.j, 0.+0.j, 0.+0.j], # may vary | |
| [0.+0.j, 0.+0.j, 0.+0.j, 1.+0.j], | |
| [0.+0.j, 0.+0.j, 1.+0.j, 0.+0.j], | |
| [0.+0.j, 1.+0.j, 0.+0.j, 0.+0.j]]) | |
| """ | |
| return _raw_fftnd(a, s, axes, ifft, norm) | |
| def rfftn(a, s=None, axes=None, norm=None): | |
| """ | |
| Compute the N-dimensional discrete Fourier Transform for real input. | |
| This function computes the N-dimensional discrete Fourier Transform over | |
| any number of axes in an M-dimensional real array by means of the Fast | |
| Fourier Transform (FFT). By default, all axes are transformed, with the | |
| real transform performed over the last axis, while the remaining | |
| transforms are complex. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array, taken to be real. | |
| s : sequence of ints, optional | |
| Shape (length along each transformed axis) to use from the input. | |
| (``s[0]`` refers to axis 0, ``s[1]`` to axis 1, etc.). | |
| The final element of `s` corresponds to `n` for ``rfft(x, n)``, while | |
| for the remaining axes, it corresponds to `n` for ``fft(x, n)``. | |
| Along any axis, if the given shape is smaller than that of the input, | |
| the input is cropped. If it is larger, the input is padded with zeros. | |
| if `s` is not given, the shape of the input along the axes specified | |
| by `axes` is used. | |
| axes : sequence of ints, optional | |
| Axes over which to compute the FFT. If not given, the last ``len(s)`` | |
| axes are used, or all axes if `s` is also not specified. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : complex ndarray | |
| The truncated or zero-padded input, transformed along the axes | |
| indicated by `axes`, or by a combination of `s` and `a`, | |
| as explained in the parameters section above. | |
| The length of the last axis transformed will be ``s[-1]//2+1``, | |
| while the remaining transformed axes will have lengths according to | |
| `s`, or unchanged from the input. | |
| Raises | |
| ------ | |
| ValueError | |
| If `s` and `axes` have different length. | |
| IndexError | |
| If an element of `axes` is larger than than the number of axes of `a`. | |
| See Also | |
| -------- | |
| irfftn : The inverse of `rfftn`, i.e. the inverse of the n-dimensional FFT | |
| of real input. | |
| fft : The one-dimensional FFT, with definitions and conventions used. | |
| rfft : The one-dimensional FFT of real input. | |
| fftn : The n-dimensional FFT. | |
| rfft2 : The two-dimensional FFT of real input. | |
| Notes | |
| ----- | |
| The transform for real input is performed over the last transformation | |
| axis, as by `rfft`, then the transform over the remaining axes is | |
| performed as by `fftn`. The order of the output is as for `rfft` for the | |
| final transformation axis, and as for `fftn` for the remaining | |
| transformation axes. | |
| See `fft` for details, definitions and conventions used. | |
| Examples | |
| -------- | |
| >>> a = np.ones((2, 2, 2)) | |
| >>> np.fft.rfftn(a) | |
| array([[[8.+0.j, 0.+0.j], # may vary | |
| [0.+0.j, 0.+0.j]], | |
| [[0.+0.j, 0.+0.j], | |
| [0.+0.j, 0.+0.j]]]) | |
| >>> np.fft.rfftn(a, axes=(2, 0)) | |
| array([[[4.+0.j, 0.+0.j], # may vary | |
| [4.+0.j, 0.+0.j]], | |
| [[0.+0.j, 0.+0.j], | |
| [0.+0.j, 0.+0.j]]]) | |
| """ | |
| a = asarray(a) | |
| s, axes = _cook_nd_args(a, s, axes) | |
| a = rfft(a, s[-1], axes[-1], norm) | |
| for ii in range(len(axes)-1): | |
| a = fft(a, s[ii], axes[ii], norm) | |
| return a | |
| def rfft2(a, s=None, axes=(-2, -1), norm=None): | |
| """ | |
| Compute the 2-dimensional FFT of a real array. | |
| Parameters | |
| ---------- | |
| a : array | |
| Input array, taken to be real. | |
| s : sequence of ints, optional | |
| Shape of the FFT. | |
| axes : sequence of ints, optional | |
| Axes over which to compute the FFT. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : ndarray | |
| The result of the real 2-D FFT. | |
| See Also | |
| -------- | |
| rfftn : Compute the N-dimensional discrete Fourier Transform for real | |
| input. | |
| Notes | |
| ----- | |
| This is really just `rfftn` with different default behavior. | |
| For more details see `rfftn`. | |
| Examples | |
| -------- | |
| >>> a = np.mgrid[:5, :5][0] | |
| >>> np.fft.rfft2(a) | |
| array([[ 50. +0.j , 0. +0.j , 0. +0.j ], | |
| [-12.5+17.20477401j, 0. +0.j , 0. +0.j ], | |
| [-12.5 +4.0614962j , 0. +0.j , 0. +0.j ], | |
| [-12.5 -4.0614962j , 0. +0.j , 0. +0.j ], | |
| [-12.5-17.20477401j, 0. +0.j , 0. +0.j ]]) | |
| """ | |
| return rfftn(a, s, axes, norm) | |
| def irfftn(a, s=None, axes=None, norm=None): | |
| """ | |
| Computes the inverse of `rfftn`. | |
| This function computes the inverse of the N-dimensional discrete | |
| Fourier Transform for real input over any number of axes in an | |
| M-dimensional array by means of the Fast Fourier Transform (FFT). In | |
| other words, ``irfftn(rfftn(a), a.shape) == a`` to within numerical | |
| accuracy. (The ``a.shape`` is necessary like ``len(a)`` is for `irfft`, | |
| and for the same reason.) | |
| The input should be ordered in the same way as is returned by `rfftn`, | |
| i.e. as for `irfft` for the final transformation axis, and as for `ifftn` | |
| along all the other axes. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| Input array. | |
| s : sequence of ints, optional | |
| Shape (length of each transformed axis) of the output | |
| (``s[0]`` refers to axis 0, ``s[1]`` to axis 1, etc.). `s` is also the | |
| number of input points used along this axis, except for the last axis, | |
| where ``s[-1]//2+1`` points of the input are used. | |
| Along any axis, if the shape indicated by `s` is smaller than that of | |
| the input, the input is cropped. If it is larger, the input is padded | |
| with zeros. If `s` is not given, the shape of the input along the axes | |
| specified by axes is used. Except for the last axis which is taken to | |
| be ``2*(m-1)`` where ``m`` is the length of the input along that axis. | |
| axes : sequence of ints, optional | |
| Axes over which to compute the inverse FFT. If not given, the last | |
| `len(s)` axes are used, or all axes if `s` is also not specified. | |
| Repeated indices in `axes` means that the inverse transform over that | |
| axis is performed multiple times. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : ndarray | |
| The truncated or zero-padded input, transformed along the axes | |
| indicated by `axes`, or by a combination of `s` or `a`, | |
| as explained in the parameters section above. | |
| The length of each transformed axis is as given by the corresponding | |
| element of `s`, or the length of the input in every axis except for the | |
| last one if `s` is not given. In the final transformed axis the length | |
| of the output when `s` is not given is ``2*(m-1)`` where ``m`` is the | |
| length of the final transformed axis of the input. To get an odd | |
| number of output points in the final axis, `s` must be specified. | |
| Raises | |
| ------ | |
| ValueError | |
| If `s` and `axes` have different length. | |
| IndexError | |
| If an element of `axes` is larger than than the number of axes of `a`. | |
| See Also | |
| -------- | |
| rfftn : The forward n-dimensional FFT of real input, | |
| of which `ifftn` is the inverse. | |
| fft : The one-dimensional FFT, with definitions and conventions used. | |
| irfft : The inverse of the one-dimensional FFT of real input. | |
| irfft2 : The inverse of the two-dimensional FFT of real input. | |
| Notes | |
| ----- | |
| See `fft` for definitions and conventions used. | |
| See `rfft` for definitions and conventions used for real input. | |
| The correct interpretation of the hermitian input depends on the shape of | |
| the original data, as given by `s`. This is because each input shape could | |
| correspond to either an odd or even length signal. By default, `irfftn` | |
| assumes an even output length which puts the last entry at the Nyquist | |
| frequency; aliasing with its symmetric counterpart. When performing the | |
| final complex to real transform, the last value is thus treated as purely | |
| real. To avoid losing information, the correct shape of the real input | |
| **must** be given. | |
| Examples | |
| -------- | |
| >>> a = np.zeros((3, 2, 2)) | |
| >>> a[0, 0, 0] = 3 * 2 * 2 | |
| >>> np.fft.irfftn(a) | |
| array([[[1., 1.], | |
| [1., 1.]], | |
| [[1., 1.], | |
| [1., 1.]], | |
| [[1., 1.], | |
| [1., 1.]]]) | |
| """ | |
| a = asarray(a) | |
| s, axes = _cook_nd_args(a, s, axes, invreal=1) | |
| for ii in range(len(axes)-1): | |
| a = ifft(a, s[ii], axes[ii], norm) | |
| a = irfft(a, s[-1], axes[-1], norm) | |
| return a | |
| def irfft2(a, s=None, axes=(-2, -1), norm=None): | |
| """ | |
| Computes the inverse of `rfft2`. | |
| Parameters | |
| ---------- | |
| a : array_like | |
| The input array | |
| s : sequence of ints, optional | |
| Shape of the real output to the inverse FFT. | |
| axes : sequence of ints, optional | |
| The axes over which to compute the inverse fft. | |
| Default is the last two axes. | |
| norm : {"backward", "ortho", "forward"}, optional | |
| .. versionadded:: 1.10.0 | |
| 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. | |
| .. versionadded:: 1.20.0 | |
| The "backward", "forward" values were added. | |
| Returns | |
| ------- | |
| out : ndarray | |
| The result of the inverse real 2-D FFT. | |
| See Also | |
| -------- | |
| rfft2 : The forward two-dimensional FFT of real input, | |
| of which `irfft2` is the inverse. | |
| rfft : The one-dimensional FFT for real input. | |
| irfft : The inverse of the one-dimensional FFT of real input. | |
| irfftn : Compute the inverse of the N-dimensional FFT of real input. | |
| Notes | |
| ----- | |
| This is really `irfftn` with different defaults. | |
| For more details see `irfftn`. | |
| Examples | |
| -------- | |
| >>> a = np.mgrid[:5, :5][0] | |
| >>> A = np.fft.rfft2(a) | |
| >>> np.fft.irfft2(A, s=a.shape) | |
| array([[0., 0., 0., 0., 0.], | |
| [1., 1., 1., 1., 1.], | |
| [2., 2., 2., 2., 2.], | |
| [3., 3., 3., 3., 3.], | |
| [4., 4., 4., 4., 4.]]) | |
| """ | |
| return irfftn(a, s, axes, norm) | |