mirror of
https://github.com/wassname/scikit-image.git
synced 2026-07-23 13:10:18 +08:00
Test and image dimension checking
This commit is contained in:
@@ -1,16 +1,45 @@
|
||||
"""
|
||||
radon.py - Radon and inverse radon transforms
|
||||
|
||||
Based on code of Justin K. Romberg
|
||||
(http://www.clear.rice.edu/elec431/projects96/DSP/bpanalysis.html)
|
||||
J. Gillam and Chris Griffin.
|
||||
|
||||
References:
|
||||
-B.R. Ramesh, N. Srinivasa, K. Rajgopal, "An Algorithm for Computing
|
||||
the Discrete Radon Transform With Some Applications", Proceedings of
|
||||
the Fourth IEEE Region 10 International Conference, TENCON '89, 1989.
|
||||
-A. C. Kak, Malcolm Slaney, "Principles of Computerized Tomographic
|
||||
Imaging", IEEE Press 1988.
|
||||
"""
|
||||
|
||||
import numpy as np
|
||||
from scipy.misc import imrotate
|
||||
from scipy.interpolate import interp1d
|
||||
from scipy.fftpack import fftshift, ifftshift, fft, ifft
|
||||
from scipy.fftpack import fftshift, fft, ifft
|
||||
import math
|
||||
|
||||
|
||||
def radon(image, theta=None):
|
||||
"""
|
||||
Calculates the projections given the current object and projection angle
|
||||
Justin K. Romberg
|
||||
Calculates the radon transform of an image given specified projection angles.
|
||||
|
||||
Parameters
|
||||
----------
|
||||
image : array_like, dtype=float
|
||||
Input image.
|
||||
theta : array_like, dtype=float, optional (default np.arange(180))
|
||||
Projection angles (in degrees).
|
||||
|
||||
Returns
|
||||
-------
|
||||
output : ndarray
|
||||
Radon transform.
|
||||
"""
|
||||
if image.ndim != 2:
|
||||
raise ValueError('The input image must be 2-D')
|
||||
if theta == None:
|
||||
theta = np.arange(180)
|
||||
theta = np.arange(180)
|
||||
height, width = image.shape
|
||||
diagonal = np.sqrt(height**2 + width**2)
|
||||
heightpad = np.ceil(diagonal - height) + 2
|
||||
@@ -25,82 +54,63 @@ def radon(image, theta=None):
|
||||
out[:,i] = rotated.sum(0)[::-1]
|
||||
return out
|
||||
|
||||
"""
|
||||
if 0:
|
||||
# filter the projections
|
||||
freqs = np.zeros((n, 1))
|
||||
freqs[:, 0] = np.linspace(-1, 1, n).T;
|
||||
filter_ft = np.tile(np.abs(freqs), (1, len(theta)))
|
||||
# fourier domain filtering
|
||||
radon_ft = fft(radon_image, axis=0)
|
||||
projection = radon_ft * fftshift(filter_ft)
|
||||
radon_filtered = np.real(ifft(projection, axis=0))
|
||||
# print np.max(projection)
|
||||
# print projection
|
||||
#projection = ifftshift(projection, axes=1);
|
||||
if 0:
|
||||
height, width = radon_image.shape
|
||||
w = np.mgrid[-math.pi:math.pi:(2*math.pi)/height]
|
||||
f = fftshift(abs(w))
|
||||
g = np.array([np.real(ifft(fft(i)*f)) for i in radon_image.T])
|
||||
radon_filtered = np.transpose(g)
|
||||
if 0:
|
||||
img = radon_image.copy()
|
||||
order = 1024
|
||||
filt = np.zeros((order/2, 1))
|
||||
filt[:, 0] = 2.0*np.arange(0, order/2)/order;
|
||||
filt = np.vstack((filt, filt[ ::-1])).T
|
||||
#filt = fftshift(abs(filt))
|
||||
# order = radon_image.shape[0]
|
||||
w = np.mgrid[-math.pi:math.pi:(2*math.pi)/order]
|
||||
filt = fftshift(abs(w))
|
||||
img.resize((order, img.shape[1]))
|
||||
radon_filtered = np.array([np.real(ifft(fft(column)*filt)) for column in img.T]).T
|
||||
radon_filtered = radon_filtered[:radon_image.shape[0], :]
|
||||
if 0:
|
||||
### bestest
|
||||
img = radon_image.copy()
|
||||
order = max(64, 2 ** np.ceil(np.log(2*n)/np.log(2)))
|
||||
# filt = np.zeros((order/2, 1))
|
||||
# filt[:, 0] = 2.0*np.arange(0, order/2)/order;
|
||||
# filt = np.vstack((filt, filt[ ::-1])).T
|
||||
#filt = fftshift(abs(filt))
|
||||
# order = radon_image.shape[0]
|
||||
w = np.mgrid[-math.pi:math.pi:(2*math.pi)/order]
|
||||
filt = fftshift(abs(w))
|
||||
img.resize((order, img.shape[1]))
|
||||
img = fft(img, axis=0)
|
||||
#radon_filtered = np.array([np.real(ifft(column*filt)) for column in img.T]).T
|
||||
radon_filtered = np.array([column*filt for column in img.T]).T
|
||||
|
||||
radon_filtered = np.real(ifft(radon_filtered, axis=0))
|
||||
radon_filtered = radon_filtered[:radon_image.shape[0], :]
|
||||
"""
|
||||
|
||||
def iradon(radon_image, theta=None, output_size=None, filter="ramp", interpolate="linear"):
|
||||
def iradon(radon_image, theta=None, output_size=None, filter="ramp", interpolation="linear"):
|
||||
"""
|
||||
Reconstructs an image from radon transformed data.
|
||||
|
||||
Parameters
|
||||
----------
|
||||
radon_image : array_like, dtype=float
|
||||
Image containing radon transform.
|
||||
theta : array_like, dtype=float, optional (default np.arange(180))
|
||||
Reconstruction angles (in degrees).
|
||||
output_size : int
|
||||
Number of rows and columns in the reconstruction.
|
||||
filter : str, optional (default ramp)
|
||||
Filter used in frequency domain filtering. Ramp filter used by default.
|
||||
Filters available: ramp, shepp-logan, cosine, hamming, hann
|
||||
Assign None to use no filter.
|
||||
interpolation : str, optional (default linear)
|
||||
Interpolation method used in reconstruction.
|
||||
Methods available: nearest, linear.
|
||||
|
||||
Returns
|
||||
-------
|
||||
output : ndarray
|
||||
Reconstructed image.
|
||||
|
||||
Notes
|
||||
-----
|
||||
It applies the fourier slice theorem to reconstruct an image by multiplying the
|
||||
frequency domain of the filter with the FFT of the projection data.
|
||||
"""
|
||||
if radon_image.ndim != 2:
|
||||
raise ValueError('The input image must be 2-D')
|
||||
if theta == None:
|
||||
theta = np.arange(180)
|
||||
th = (math.pi/180.0)*theta
|
||||
# if output size not specified, estimate from input radon image
|
||||
if not output_size:
|
||||
output_size = 2*np.floor(radon_image.shape[0] / (2*np.sqrt(2)))
|
||||
output_size = 2*np.floor(radon_image.shape[0] / (2 * np.sqrt(2)))
|
||||
n = radon_image.shape[0]
|
||||
|
||||
img = radon_image.copy()
|
||||
# resize image to next power of two for fourier analysis
|
||||
order = max(64, 2 ** np.ceil(np.log(2*n)/np.log(2)))
|
||||
# speeds up fourier and lessens artifacts
|
||||
order = max(64, 2 ** np.ceil(np.log(2 * n) / np.log(2)))
|
||||
# zero pad input image
|
||||
img.resize((order, img.shape[1]))
|
||||
#construct the fourier filter
|
||||
freqs = np.zeros((order, 1))
|
||||
|
||||
f = fftshift(abs(np.mgrid[-1:1:2/order])).reshape(-1, 1)
|
||||
f = fftshift(abs(np.mgrid[-1:1:2 / order])).reshape(-1, 1)
|
||||
w = 2 * math.pi * f
|
||||
# start from first element to avoid divide by zero
|
||||
if filter == "ramp":
|
||||
pass
|
||||
elif filter == "shepp-logan":
|
||||
f[1:] = f[1:] * np.sin(w[1:] / 2) / (w[1:]/2)
|
||||
f[1:] = f[1:] * np.sin(w[1:] / 2) / (w[1:] / 2)
|
||||
elif filter == "cosine":
|
||||
f[1:] = f[1:] * np.cos(w[1:] / 2)
|
||||
elif filter == "hamming":
|
||||
@@ -125,30 +135,32 @@ def iradon(radon_image, theta=None, output_size=None, filter="ramp", interpolate
|
||||
[X, Y] = np.mgrid[0.0:x, 0.0:y]
|
||||
xpr = X - (output_size + 1.0) / 2.0
|
||||
ypr = Y - (output_size + 1.0) / 2.0
|
||||
if interpolate == "nearest":
|
||||
|
||||
# reconstruct image by interpolation
|
||||
if interpolation == "nearest":
|
||||
for i in range(len(theta)):
|
||||
k = np.round(mid_index + xpr*np.sin(th[i]) - ypr*np.cos(th[i]))
|
||||
reconstructed += radon_filtered[((((k > 0) & (k < n))*k) - 1).astype(np.int), i]
|
||||
elif interpolate == "linear":
|
||||
elif interpolation == "linear":
|
||||
for i in range(len(theta)):
|
||||
t = xpr*np.sin(th[i]) - ypr*np.cos(th[i])
|
||||
a = np.floor(t)
|
||||
b = mid_index + a
|
||||
reconstructed += (t - a) * radon_filtered[((((b+1 > 0) & (b+1 < n))*(b+1)) - 1).astype(np.int), i] \
|
||||
+ (a - t + 1) * radon_filtered[((((b > 0) & (b < n))*b) - 1).astype(np.int), i]
|
||||
# XXX slow and inaccurate
|
||||
# elif interpolate == "spline":
|
||||
b0 = ((((b + 1 > 0) & (b + 1 < n))*(b + 1)) - 1).astype(np.int)
|
||||
b1 = ((((b > 0) & (b < n))*b) - 1).astype(np.int)
|
||||
reconstructed += (t - a) * radon_filtered[b0, i] + (a - t + 1) * radon_filtered[b1, i]
|
||||
# XXX slow with some artifacts
|
||||
# elif interpolation == "spline":
|
||||
# axis = np.arange(0, radon_filtered.shape[0]) - mid_index
|
||||
# for i in range(len(theta)):
|
||||
# print i
|
||||
# t = xpr*np.sin(th[i]) - ypr*np.cos(th[i])
|
||||
# #f = interp1d(axis, radon_filtered[:, i], kind="cubic", bounds_error=False, fill_value=0)
|
||||
# f = interp1d(axis, radon_filtered[:, i], kind="linear", bounds_error=False, fill_value=0) # cubic
|
||||
# f = interp1d(axis, radon_filtered[:, i], kind="linear", bounds_error=False, fill_value=0)
|
||||
# reconstructed += f(t).reshape(output_size, output_size)
|
||||
else:
|
||||
raise ValueError("Unknown interpolation: %s" % interpolate)
|
||||
raise ValueError("Unknown interpolation: %s" % interpolation)
|
||||
|
||||
return reconstructed * math.pi / (2*len(th))
|
||||
|
||||
|
||||
|
||||
|
||||
@@ -0,0 +1,20 @@
|
||||
import numpy as np
|
||||
from numpy.testing import *
|
||||
from scikits.image.transform import *
|
||||
|
||||
|
||||
def test_radon_iradon():
|
||||
size = 100
|
||||
image = np.tri(size) + np.tri(size)[::-1]
|
||||
for filter_type in ["ramp", "shepp-logan", "cosine", "hamming", "hann"]:
|
||||
reconstructed = iradon(radon(image), filter=filter_type)
|
||||
delta = np.sum(abs(image/np.max(image) - reconstructed/np.max(reconstructed)))/(size*size)
|
||||
assert delta < 0.1
|
||||
reconstructed = iradon(radon(image), filter="ramp", interpolation="nearest")
|
||||
delta = np.sum(abs(image/np.max(image) - reconstructed/np.max(reconstructed)))/(size*size)
|
||||
assert delta < 0.1
|
||||
|
||||
|
||||
if __name__ == "__main__":
|
||||
run_module_suite()
|
||||
|
||||
Reference in New Issue
Block a user