SciPy - ifftn() Function



The scipy.fft.ifftn() method gives the N-dimensional Inverse Fast Fourier Transform for complex data by transforming frequency domain data to spatial or time domain on 1D, 2D, 3D or more.

This method is extensively used in reconstructing multi-dimensional signals that are in the form of 2D pictures and 3D volumetric data-for instance, in the field of medical imaging. It is suited for applications requiring higher-dimensional data.

The ifftn method is a generalized IFFT for N-dimensions, that include 2D, 3D, and more so it is applicable to multidimensional data. In contrast, ifft handles a 1D data input like time series. Whereas, ifft2 specifically deals with 2-dimensional data like pictures or matrices.

Syntax

The syntax for the SciPy ifftn() method is as follows −

.ifftn(x, s=None, axes=None, norm=None, overwrite_x=False, workers=None, *, plan=None)

Parameters

This method accepts the following parameters −

  • x (array_like) − Input array (can be complex) representing data in the frequency domain.

  • s (sequence of ints, optional) − Shape of the output along each transformed axis. Pads with zeros or truncates the input.

  • axes (sequence of ints, optional) − Axes over which to compute the IFFT. Defaults to all axes.

  • norm (str, optional) − The normalization mode allows control over scaling: "backward" (default, no scaling), "ortho" (unitary scaling for energy preservation), and "forward" (scales the output by 1/n, where n is the transform length).

  • overwrite_x (bool, optional) − If True, allows the input array x to be overwritten for better performance. Default is False.

  • workers (str, optional) − Number of parallel workers to use for computation. Default is None, meaning a single thread is used.

  • plan (optional) − Precomputed plan for FFT optimization (advanced use). Default is None.

Return Value

out The N-dimensional IFFT result, representing reconstructed data in the spatial or time domain.

Example 1

This is an example of a simple reconstruction of the data. This is performed first by transforming the data to the frequency domain through FFT fftn() and then returning to the original spatial domain through the IFFT ifftn().

import numpy as np
from scipy.fft import fftn, ifftn

# Create a 2D array
x = np.array([[1, 2], [3, 4]])

# Perform FFT and then IFFT
freq = fftn(x)
reconstructed = ifftn(freq).real

print("Reconstructed Data:\n", reconstructed)

When we run above program, it produces following result

Reconstructed Data:
 [[1. 2.]
 [3. 4.]]

Example 2

The below code creates an image with specific frequency content by specifying a small set of active frequencies in a 2D frequency domain. These frequencies are translated back into the spatial domain by ifftn() method, and the result is a periodic pattern in the image.

The output is a grayscale image with patterns matching to the frequencies that were triggered. Narrow frequency bands produce grid-like periodic structures, illustrating how changes in the frequency domain are translated into spatial domain images.

import numpy as np
import matplotlib.pyplot as plt
from scipy.fft import ifftn

# Create a band-limited frequency domain
n = np.zeros((200, 200), dtype=complex)  # Create a 2D frequency domain with zeros
n[50:70, 30:50] = np.exp(1j * np.random.uniform(0, 2 * np.pi, (20, 20)))  # Add random phase content

# Transform back to the spatial domain using Inverse FFT
im = ifftn(n).real

# Plot the resulting image
plt.imshow(im, cmap='gray')
plt.title("Image with Band-Limited Frequency Content")
plt.colorbar()
plt.show()
scipy_discrete_fourier_transform.htm
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