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3.18 kB
| """ | |
| :author: Gary Ruben, 2009 | |
| :license: modified BSD | |
| """ | |
| __all__ = ["frt2", "ifrt2"] | |
| import numpy as np | |
| from numpy import roll, newaxis | |
| def frt2(a): | |
| """Compute the 2-dimensional finite Radon transform (FRT) for the input array. | |
| Parameters | |
| ---------- | |
| a : ndarray of int, shape (M, M) | |
| Input array. | |
| Returns | |
| ------- | |
| FRT : ndarray of int, shape (M+1, M) | |
| Finite Radon Transform array of coefficients. | |
| See Also | |
| -------- | |
| ifrt2 : The two-dimensional inverse FRT. | |
| Notes | |
| ----- | |
| The FRT has a unique inverse if and only if M is prime. [FRT] | |
| The idea for this algorithm is due to Vlad Negnevitski. | |
| Examples | |
| -------- | |
| Generate a test image: | |
| Use a prime number for the array dimensions | |
| >>> SIZE = 59 | |
| >>> img = np.tri(SIZE, dtype=np.int32) | |
| Apply the Finite Radon Transform: | |
| >>> f = frt2(img) | |
| References | |
| ---------- | |
| .. [FRT] A. Kingston and I. Svalbe, "Projective transforms on periodic | |
| discrete image arrays," in P. Hawkes (Ed), Advances in Imaging | |
| and Electron Physics, 139 (2006) | |
| """ | |
| if a.ndim != 2 or a.shape[0] != a.shape[1]: | |
| raise ValueError("Input must be a square, 2-D array") | |
| ai = a.copy() | |
| n = ai.shape[0] | |
| f = np.empty((n + 1, n), np.uint32) | |
| f[0] = ai.sum(axis=0) | |
| for m in range(1, n): | |
| # Roll the pth row of ai left by p places | |
| for row in range(1, n): | |
| ai[row] = roll(ai[row], -row) | |
| f[m] = ai.sum(axis=0) | |
| f[n] = ai.sum(axis=1) | |
| return f | |
| def ifrt2(a): | |
| """Compute the 2-dimensional inverse finite Radon transform (iFRT) for the input array. | |
| Parameters | |
| ---------- | |
| a : ndarray of int, shape (M+1, M) | |
| Input array. | |
| Returns | |
| ------- | |
| iFRT : ndarray of int, shape (M, M) | |
| Inverse Finite Radon Transform coefficients. | |
| See Also | |
| -------- | |
| frt2 : The two-dimensional FRT | |
| Notes | |
| ----- | |
| The FRT has a unique inverse if and only if M is prime. | |
| See [1]_ for an overview. | |
| The idea for this algorithm is due to Vlad Negnevitski. | |
| Examples | |
| -------- | |
| >>> SIZE = 59 | |
| >>> img = np.tri(SIZE, dtype=np.int32) | |
| Apply the Finite Radon Transform: | |
| >>> f = frt2(img) | |
| Apply the Inverse Finite Radon Transform to recover the input | |
| >>> fi = ifrt2(f) | |
| Check that it's identical to the original | |
| >>> assert len(np.nonzero(img-fi)[0]) == 0 | |
| References | |
| ---------- | |
| .. [1] A. Kingston and I. Svalbe, "Projective transforms on periodic | |
| discrete image arrays," in P. Hawkes (Ed), Advances in Imaging | |
| and Electron Physics, 139 (2006) | |
| """ | |
| if a.ndim != 2 or a.shape[0] != a.shape[1] + 1: | |
| raise ValueError("Input must be an (n+1) row x n column, 2-D array") | |
| ai = a.copy()[:-1] | |
| n = ai.shape[1] | |
| f = np.empty((n, n), np.uint32) | |
| f[0] = ai.sum(axis=0) | |
| for m in range(1, n): | |
| # Rolls the pth row of ai right by p places. | |
| for row in range(1, ai.shape[0]): | |
| ai[row] = roll(ai[row], row) | |
| f[m] = ai.sum(axis=0) | |
| f += a[-1][newaxis].T | |
| f = (f - ai[0].sum()) / n | |
| return f | |