linting test_image_processing.py and test_initializers.py

This commit is contained in:
gnzng
2025-07-07 14:40:17 -07:00
parent b00f39e1fe
commit 88df4c0794
2 changed files with 115 additions and 124 deletions
+58 -66
View File
@@ -1,26 +1,27 @@
from cdtools.tools import initializers
from cdtools.datasets import Ptycho2DDataset
import numpy as np
import torch as t
from cdtools.tools import initializers
from cdtools.datasets import Ptycho2DDataset
def test_exit_wave_geometry():
# First test a simple case where nothing need change
basis = t.Tensor([[0,-30e-6,0],
[-20e-6,0,0]]).transpose(0,1)
shape = t.Size([73,56])
basis = t.Tensor([[0, -30e-6, 0],
[-20e-6, 0, 0]]).transpose(0, 1)
shape = t.Size([73, 56])
wavelength = 1e-9
distance = 1.
rs_basis = initializers.exit_wave_geometry(basis, shape, wavelength, distance)
assert t.allclose(rs_basis[0,1],t.Tensor([-8.928571428571428e-07]))
assert t.allclose(rs_basis[1,0],t.Tensor([-4.5662100456621004e-07]))
assert t.allclose(rs_basis[0, 1], t.Tensor([-8.928571428571428e-07]))
assert t.allclose(rs_basis[1, 0], t.Tensor([-4.5662100456621004e-07]))
def test_calc_object_setup():
# First just try a simple case
probe_shape = t.Size([120,57])
translations = t.rand((30,2)) * 300
probe_shape = t.Size([120, 57])
translations = t.rand((30, 2)) * 300
t_max = t.max(translations, dim=0)[0]
t_min = t.min(translations, dim=0)[0]
obj_shape, min_translation = initializers.calc_object_setup(probe_shape, translations)
@@ -28,65 +29,58 @@ def test_calc_object_setup():
assert t.allclose(min_translation, t_min)
assert obj_shape == t.Size(exp_shape)
# Then add some padding
padding = 5
obj_shape, min_translation = initializers.calc_object_setup(probe_shape, translations, padding=padding)
assert t.allclose(min_translation, t_min - padding)
assert obj_shape == t.Size(exp_shape + 2 * padding)
def test_gaussian():
# Generate gaussian as a numpy array (square array)
shape = [10, 10]
sigma = [2.5, 2.5]
center = ((shape[0]-1)/2, (shape[1]-1)/2)
center = ((shape[0] - 1) / 2, (shape[1] - 1) / 2)
y, x = np.mgrid[:shape[0], :shape[1]]
np_result = 10*np.exp(-0.5*((x-center[1])/sigma[1])**2
-0.5*((y-center[0])/sigma[0])**2)
np_result = 10 * np.exp(-0.5 * ((x - center[1]) / sigma[1])**2 - 0.5 * ((y - center[0]) / sigma[0])**2)
init_result = initializers.gaussian(shape, sigma, amplitude=10).numpy()
assert np.allclose(init_result, np_result)
# Generate gaussian as a numpy array (rectangular array)
shape = [10, 5]
sigma = [2.5, 3]
center = ((shape[0]-1)/2, (shape[1]-1)/2)
center = ((shape[0] - 1) / 2, (shape[1] - 1) / 2)
y, x = np.mgrid[:shape[0], :shape[1]]
np_result = np.exp(-0.5*((x-center[1])/sigma[1])**2
-0.5*((y-center[0])/sigma[0])**2)
np_result = np.exp(-0.5 * ((x - center[1]) / sigma[1])**2
- 0.5 * ((y - center[0]) / sigma[0])**2)
init_result = initializers.gaussian(shape, sigma).numpy()
assert np.allclose(init_result, np_result)
# Generate gaussian with curvature
shape = [20, 30]
sigma = [2.5, 5]
curvature = [1,0.6]
center = ((shape[0]-1)/2 + 3, (shape[1]-1)/2 - 1.4)
curvature = [1, 0.6]
center = ((shape[0] - 1) / 2 + 3, (shape[1] - 1) / 2 - 1.4)
y, x = np.mgrid[:shape[0], :shape[1]]
np_result = (10+0j)*np.exp(-0.5*((x-center[1])/sigma[1])**2
-0.5*((y-center[0])/sigma[0])**2)
np_result *= np.exp(0.5j*curvature[1]*(x-center[1])**2
+0.5j*curvature[0]*(y-center[0])**2)
init_result = initializers.gaussian(shape, sigma, center=center,
curvature=curvature, amplitude=10).numpy()
np_result = (10 + 0j) * np.exp(-0.5 * ((x - center[1]) / sigma[1])**2 - 0.5 * ((y - center[0]) / sigma[0])**2)
np_result *= np.exp(0.5j * curvature[1] * (x - center[1])**2 + 0.5j * curvature[0] * (y - center[0])**2)
init_result = initializers.gaussian(shape, sigma, center=center, curvature=curvature, amplitude=10).numpy()
assert np.allclose(init_result, np_result)
def test_gaussian_probe(ptycho_cxi_1):
dataset = Ptycho2DDataset.from_cxi(ptycho_cxi_1[0])
det_basis = t.Tensor(dataset.detector_geometry['basis'])
det_shape = t.Size(dataset.patterns.shape[-2:])
wavelength = dataset.wavelength
distance = dataset.detector_geometry['distance']
basis = initializers.exit_wave_geometry(det_basis,
det_shape,
wavelength,
distance)
det_shape,
wavelength,
distance)
# Basis is around 60nm in the i(y) direction, 85nm in the j(x) direction
# Full window is therefore about 15 um in i(y) and 20 um in the j(x) dir
@@ -94,15 +88,13 @@ def test_gaussian_probe(ptycho_cxi_1):
sigma = 5e-7
# Build a stage explicitly with numpy to compare against
x = (np.arange(256) - 127.5) * (-basis[0,1]).numpy()
y = (np.arange(256) - 127.5) * (-basis[1,0]).numpy()
Xs,Ys = np.meshgrid(x,y)
Rs = np.sqrt(Xs**2+Ys**2)
x = (np.arange(256) - 127.5) * (-basis[0, 1]).numpy()
y = (np.arange(256) - 127.5) * (-basis[1, 0]).numpy()
Xs, Ys = np.meshgrid(x, y)
Rs = np.sqrt(Xs**2 + Ys**2)
# Now we first test the non-propagated probe
np_probe = np.exp(-1/(2*sigma**2) * Rs**2)
np_probe = np.exp(- 1 / (2 * sigma**2) * Rs**2)
normalization = 0
for params, im in dataset:
@@ -110,27 +102,26 @@ def test_gaussian_probe(ptycho_cxi_1):
normalization /= len(dataset)
normalization_1 = np.sqrt(normalization / np.sum(np.abs(np_probe)**2))
probe = initializers.gaussian_probe(
dataset, basis, det_shape, sigma).numpy()
assert np.allclose(probe, normalization_1*np_probe)
assert np.allclose(probe, normalization_1 * np_probe)
# And then a propagated probe
z = 1e-4 #nm
z = 1e-4 # nm
k = 2 * np.pi / wavelength
w0 = np.sqrt(2)*sigma
w0 = np.sqrt(2) * sigma
zr = np.pi * w0**2 / wavelength
wz = w0 * np.sqrt(1 + (z / zr)**2)
Rz = z * (1 + (zr / z)**2)
np_probe = np.exp(-Rs**2 / wz**2) * np.exp(-1j * k * Rs**2 / (2 * Rz))
Rz = z * (1 + (zr / z)**2)
np_probe = np.exp(-Rs**2 / wz**2) * np.exp(-1j * k * Rs**2 / (2 * Rz))
normalization_2 = np.sqrt(normalization / np.sum(np.abs(np_probe)**2))
normalization_2 = np.sqrt(normalization / np.sum(np.abs(np_probe)**2))
probe = initializers.gaussian_probe(dataset, basis, det_shape, sigma,
propagation_distance=z).numpy()
assert np.allclose(probe, normalization_2*np_probe)
assert np.allclose(probe, normalization_2 * np_probe)
def test_SHARP_style_probe(ptycho_cxi_1):
@@ -148,11 +139,13 @@ def test_SHARP_style_probe(ptycho_cxi_1):
wavelength,
distance)
assert basis.shape == t.Size([3, 2])
probe = initializers.SHARP_style_probe(dataset)
assert probe.shape == t.Size([256,256])
assert probe.shape == t.Size([256, 256])
probe = initializers.SHARP_style_probe(dataset, propagation_distance=20e-6)
assert probe.shape == t.Size([256,256])
assert probe.shape == t.Size([256, 256])
def test_RPI_spectral_init():
@@ -160,28 +153,27 @@ def test_RPI_spectral_init():
# since the original implementation is in numpy and there aren't any clear
# cases that can be calculated analytically.
pattern = np.random.rand(230,253).astype(np.float32)
probe = np.random.rand(230,253).astype(np.complex64)
obj_shape = [37,53]
pattern = np.random.rand(230, 253).astype(np.float32)
probe = np.random.rand(230, 253).astype(np.complex64)
obj_shape = [37, 53]
mask = t.Tensor(np.random.rand(*pattern.shape) > 0.04)
background = t.as_tensor(np.random.rand(*pattern.shape),dtype=t.float32) * 0.05
background = t.as_tensor(np.random.rand(*pattern.shape), dtype=t.float32) * 0.05
probe = t.as_tensor(probe)
pattern = t.as_tensor(pattern)
obj = initializers.RPI_spectral_init(pattern, probe, obj_shape)
assert list(obj.shape) == [1]+obj_shape
assert list(obj.shape) == [1] + obj_shape
obj = initializers.RPI_spectral_init(pattern, probe, obj_shape,
n_modes=2, mask=mask)
assert list(obj.shape) == [2]+obj_shape
assert list(obj.shape) == [2] + obj_shape
obj = initializers.RPI_spectral_init(pattern, probe, obj_shape,
n_modes=2, background=background)
assert list(obj.shape) == [2]+obj_shape
assert list(obj.shape) == [2] + obj_shape
obj = initializers.RPI_spectral_init(pattern, probe, obj_shape,
n_modes=2, mask=mask,
background=background)
assert list(obj.shape) == [2]+obj_shape
assert list(obj.shape) == [2] + obj_shape