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[core] Fix spatial derivatives when using mode='bspline' or 'gaussian'
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r"""Interactive test and visualization of vector flow derivatives.""" | ||
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# %% | ||
# Imports | ||
from typing import Dict, Optional, Sequence | ||
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import matplotlib.pyplot as plt | ||
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import torch | ||
from torch import Tensor | ||
from torch.random import Generator | ||
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from deepali.core import Axes, Grid | ||
import deepali.core.bspline as B | ||
import deepali.core.functional as U | ||
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# %% | ||
# Auxiliary functions | ||
def change_axes(flow: Tensor, grid: Grid, axes: Axes, to_axes: Axes) -> Tensor: | ||
if axes != to_axes: | ||
flow = U.move_dim(flow, 1, -1) | ||
flow = grid.transform_vectors(flow, axes=axes, to_axes=to_axes) | ||
flow = U.move_dim(flow, -1, 1) | ||
return flow | ||
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def flow_derivatives( | ||
flow: Tensor, grid: Grid, axes: Axes, to_axes: Optional[Axes] = None, **kwargs | ||
) -> Dict[str, Tensor]: | ||
if to_axes is None: | ||
to_axes = axes | ||
flow = change_axes(flow, grid, axes, to_axes) | ||
axes = to_axes | ||
if "spacing" not in kwargs: | ||
if axes == Axes.CUBE: | ||
spacing = tuple(2 / n for n in grid.size()) | ||
elif axes == Axes.CUBE_CORNERS: | ||
spacing = tuple(2 / (n - 1) for n in grid.size()) | ||
elif axes == Axes.GRID: | ||
spacing = 1 | ||
elif axes == Axes.WORLD: | ||
spacing = grid.spacing() | ||
else: | ||
spacing = None | ||
kwargs["spacing"] = spacing | ||
return U.flow_derivatives(flow, **kwargs) | ||
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def random_svf( | ||
size: Sequence[int], | ||
stride: int = 1, | ||
generator: Optional[Generator] = None, | ||
) -> Tensor: | ||
cp_grid_size = B.cubic_bspline_control_point_grid_size(size, stride=stride) | ||
cp_grid_size = tuple(reversed(cp_grid_size)) | ||
data = torch.randn((1, 3) + cp_grid_size, generator=generator) | ||
data = U.fill_border(data, margin=3, value=0, inplace=True) | ||
return B.evaluate_cubic_bspline(data, size=size, stride=stride) | ||
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def visualize_flow( | ||
ax: plt.Axes, | ||
flow: Tensor, | ||
grid: Optional[Grid] = None, | ||
axes: Optional[Axes] = None, | ||
label: Optional[str] = None, | ||
) -> None: | ||
if grid is None: | ||
grid = Grid(shape=flow.shape[2:]) | ||
if axes is None: | ||
axes = grid.axes() | ||
flow = change_axes(flow, grid, axes, grid.axes()) | ||
x = grid.coords(channels_last=False, dtype=flow.dtype, device=flow.device) | ||
x = U.move_dim(x.unsqueeze_(0).add_(flow), 1, -1) | ||
target_grid = U.grid_image(shape=flow.shape[2:], inverted=True, stride=(5, 5)) | ||
warped_grid = U.warp_image(target_grid, x, align_corners=grid.align_corners()) | ||
ax.imshow(warped_grid[0, 0, flow.shape[2] // 2], cmap="gray") | ||
if label: | ||
ax.set_title(label, fontsize=24) | ||
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# %% | ||
# Random velocity fields | ||
generator = torch.Generator().manual_seed(42) | ||
grid = Grid(size=(128, 128, 64), spacing=(0.5, 0.5, 1.0)) | ||
flow = random_svf(grid.size(), stride=8, generator=generator).mul_(0.1) | ||
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fig, axes = plt.subplots(1, 1, figsize=(4, 4)) | ||
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ax = axes | ||
ax.set_title("v", fontsize=24, pad=20) | ||
visualize_flow(ax, flow, grid=grid, axes=grid.axes()) | ||
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# %% | ||
# Visualise first order derivatives for different modes | ||
configs = [ | ||
dict(mode="forward_central_backward"), | ||
dict(mode="bspline"), | ||
dict(mode="gaussian", sigma=0.7355), | ||
] | ||
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fig, axes = plt.subplots(len(configs), 4, figsize=(16, 4 * len(configs))) | ||
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for i, config in enumerate(configs): | ||
derivs = flow_derivatives( | ||
flow, | ||
grid=grid, | ||
axes=grid.axes(), | ||
to_axes=Axes.GRID, | ||
which=["du/dx", "du/dy", "dv/dx", "dv/dy"], | ||
**config, | ||
) | ||
for ax, (key, deriv) in zip(axes[i], derivs.items()): | ||
if i == 0: | ||
ax.set_title(key, fontsize=24, pad=20) | ||
ax.imshow(deriv[0, 0, deriv.shape[2] // 2], vmin=-1, vmax=1) | ||
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# %% | ||
# Compare magnitudes of first order derivatives for different modes | ||
flow_axes = [Axes.GRID, Axes.WORLD, Axes.CUBE_CORNERS] | ||
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sigma = 0.7355 | ||
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configs = [ | ||
dict(mode="bspline"), | ||
dict(mode="gaussian", sigma=sigma), | ||
dict(mode="forward_central_backward", sigma=sigma), | ||
dict(mode="forward_central_backward"), | ||
] | ||
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for to_axes in flow_axes: | ||
for config in configs: | ||
print(f"axes={to_axes}, " + ", ".join(f"{k}={v!r}" for k, v in config.items())) | ||
derivs = flow_derivatives( | ||
flow, | ||
grid=grid, | ||
axes=grid.axes(), | ||
to_axes=to_axes, | ||
which=["du/dx", "du/dy", "dv/dx", "dv/dy"], | ||
**config, | ||
) | ||
for key, deriv in derivs.items(): | ||
print(f"- max(abs({key})): {deriv.abs().max().item():.5f}") | ||
print() | ||
print("\n") | ||
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# %% | ||
# Visualise second order derivatives for different modes | ||
configs = [ | ||
dict(mode="forward_central_backward"), | ||
dict(mode="bspline"), | ||
dict(mode="gaussian", sigma=0.7355), | ||
] | ||
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fig, axes = plt.subplots(len(configs), 4, figsize=(16, 4 * len(configs))) | ||
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for i, config in enumerate(configs): | ||
derivs = flow_derivatives( | ||
flow, | ||
grid=grid, | ||
axes=grid.axes(), | ||
to_axes=Axes.GRID, | ||
which=["du/dxx", "du/dxy", "dv/dxy", "dv/dyy"], | ||
**config, | ||
) | ||
for ax, (key, deriv) in zip(axes[i], derivs.items()): | ||
if i == 0: | ||
ax.set_title(key, fontsize=24, pad=20) | ||
ax.imshow(deriv[0, 0, deriv.shape[2] // 2], vmin=-0.4, vmax=0.4) | ||
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# %% | ||
# Compare magnitudes of second order derivatives for different modes | ||
flow_axes = [Axes.GRID, Axes.WORLD, Axes.CUBE_CORNERS] | ||
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sigma = 0.7355 | ||
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configs = [ | ||
dict(mode="bspline"), | ||
dict(mode="gaussian", sigma=sigma), | ||
dict(mode="forward_central_backward", sigma=sigma), | ||
dict(mode="forward_central_backward"), | ||
] | ||
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for to_axes in flow_axes: | ||
for config in configs: | ||
print(f"axes={to_axes}, " + ", ".join(f"{k}={v!r}" for k, v in config.items())) | ||
derivs = flow_derivatives( | ||
flow, | ||
grid=grid, | ||
axes=grid.axes(), | ||
to_axes=to_axes, | ||
which=["du/dxx", "du/dxy", "dv/dxy", "dv/dyy"], | ||
**config, | ||
) | ||
for key, deriv in derivs.items(): | ||
print(f"- max(abs({key})): {deriv.abs().max().item():.5f}") | ||
print() | ||
print("\n") | ||
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# %% |