def v_cycle_2d(n, k, delta_field, sigma_sq_field, gradient_field, target,
lambda_param, displacement, depth=0):
r"""Multi-resolution Gauss-Seidel solver using V-type cycles
Multi-resolution Gauss-Seidel solver: solves the Gauss-Newton linear system
by first filtering (GS-iterate) the current level, then solves for the
residual at a coarser resolution and finally refines the solution at the
current resolution. This scheme corresponds to the V-cycle proposed by
Bruhn and Weickert[Bruhn05].
Parameters
----------
n : int
number of levels of the multi-resolution algorithm (it will be called
recursively until level n == 0)
k : int
the number of iterations at each multi-resolution level
delta_field : array, shape (R, C)
the difference between the static and moving image (the 'derivative
w.r.t. time' in the optical flow model)
sigma_sq_field : array, shape (R, C)
the variance of the gray level value at each voxel, according to the
EM model (for SSD, it is 1 for all voxels). Inf and 0 values
are processed specially to support infinite and zero variance.
gradient_field : array, shape (R, C, 2)
the gradient of the moving image
target : array, shape (R, C, 2)
right-hand side of the linear system to be solved in the Weickert's
multi-resolution algorithm
lambda_param : float
smoothness parameter, the larger its value the smoother the
displacement field
displacement : array, shape (R, C, 2)
the displacement field to start the optimization from
Returns
-------
energy : the energy of the EM (or SSD if sigmafield[...]==1) metric at this
iteration
References
----------
[Bruhn05] Andres Bruhn and Joachim Weickert, "Towards ultimate motion
estimation: combining highest accuracy with real-time
performance", 10th IEEE International Conference on Computer
Vision, 2005. ICCV 2005.
"""
# pre-smoothing
for i in range(k):
ssd.iterate_residual_displacement_field_ssd_2d(delta_field,
sigma_sq_field,
gradient_field,
target,
lambda_param,
displacement)
if n == 0:
energy = ssd.compute_energy_ssd_2d(delta_field)
return energy
# solve at coarser grid
residual = None
residual = ssd.compute_residual_displacement_field_ssd_2d(delta_field,
sigma_sq_field,
gradient_field,
target,
lambda_param,
displacement,
residual)
sub_residual = np.array(vfu.downsample_displacement_field_2d(residual))
del residual
subsigma_sq_field = None
if sigma_sq_field is not None:
subsigma_sq_field = vfu.downsample_scalar_field_2d(sigma_sq_field)
subdelta_field = vfu.downsample_scalar_field_2d(delta_field)
subgradient_field = np.array(
vfu.downsample_displacement_field_2d(gradient_field))
shape = np.array(displacement.shape).astype(np.int32)
half_shape = ((shape[0] + 1) // 2, (shape[1] + 1) // 2, 2)
sub_displacement = np.zeros(shape=half_shape,
dtype=floating)
sublambda_param = lambda_param*0.25
v_cycle_2d(n-1, k, subdelta_field, subsigma_sq_field, subgradient_field,
sub_residual, sublambda_param, sub_displacement, depth+1)
# displacement += np.array(
# vfu.upsample_displacement_field(sub_displacement, shape))
displacement += vfu.resample_displacement_field_2d(sub_displacement,
np.array([0.5, 0.5]),
shape)
# post-smoothing
for i in range(k):
ssd.iterate_residual_displacement_field_ssd_2d(delta_field,
sigma_sq_field,
gradient_field,
target,
lambda_param,
displacement)
energy = ssd.compute_energy_ssd_2d(delta_field)
return energy
def v_cycle_2d(n,
k,
delta_field,
sigma_sq_field,
gradient_field,
target,
lambda_param,
displacement,
depth=0):
r"""Multi-resolution Gauss-Seidel solver using V-type cycles
Multi-resolution Gauss-Seidel solver: solves the Gauss-Newton linear system
by first filtering (GS-iterate) the current level, then solves for the
residual at a coarser resolution and finally refines the solution at the
current resolution. This scheme corresponds to the V-cycle proposed by
Bruhn and Weickert[Bruhn05].
Parameters
----------
n : int
number of levels of the multi-resolution algorithm (it will be called
recursively until level n == 0)
k : int
the number of iterations at each multi-resolution level
delta_field : array, shape (R, C)
the difference between the static and moving image (the 'derivative
w.r.t. time' in the optical flow model)
sigma_sq_field : array, shape (R, C)
the variance of the gray level value at each voxel, according to the
EM model (for SSD, it is 1 for all voxels). Inf and 0 values
are processed specially to support infinite and zero variance.
gradient_field : array, shape (R, C, 2)
the gradient of the moving image
target : array, shape (R, C, 2)
right-hand side of the linear system to be solved in the Weickert's
multi-resolution algorithm
lambda_param : float
smoothness parameter, the larger its value the smoother the
displacement field
displacement : array, shape (R, C, 2)
the displacement field to start the optimization from
Returns
-------
energy : the energy of the EM (or SSD if sigmafield[...]==1) metric at this
iteration
References
----------
[Bruhn05] Andres Bruhn and Joachim Weickert, "Towards ultimate motion
estimation: combining highest accuracy with real-time
performance", 10th IEEE International Conference on Computer
Vision, 2005. ICCV 2005.
"""
# pre-smoothing
for i in range(k):
ssd.iterate_residual_displacement_field_ssd_2d(delta_field,
sigma_sq_field,
gradient_field, target,
lambda_param,
displacement)
if n == 0:
energy = ssd.compute_energy_ssd_2d(delta_field)
return energy
# solve at coarser grid
residual = None
residual = ssd.compute_residual_displacement_field_ssd_2d(
delta_field, sigma_sq_field, gradient_field, target, lambda_param,
displacement, residual)
sub_residual = np.array(vfu.downsample_displacement_field_2d(residual))
del residual
subsigma_sq_field = None
if sigma_sq_field is not None:
subsigma_sq_field = vfu.downsample_scalar_field_2d(sigma_sq_field)
subdelta_field = vfu.downsample_scalar_field_2d(delta_field)
subgradient_field = np.array(
vfu.downsample_displacement_field_2d(gradient_field))
shape = np.array(displacement.shape).astype(np.int32)
half_shape = ((shape[0] + 1) // 2, (shape[1] + 1) // 2, 2)
sub_displacement = np.zeros(shape=half_shape, dtype=floating)
sublambda_param = lambda_param * 0.25
v_cycle_2d(n - 1, k, subdelta_field, subsigma_sq_field, subgradient_field,
sub_residual, sublambda_param, sub_displacement, depth + 1)
# displacement += np.array(
# vfu.upsample_displacement_field(sub_displacement, shape))
displacement += vfu.resample_displacement_field_2d(sub_displacement,
np.array([0.5, 0.5]),
shape)
# post-smoothing
for i in range(k):
ssd.iterate_residual_displacement_field_ssd_2d(delta_field,
sigma_sq_field,
gradient_field, target,
lambda_param,
displacement)
energy = ssd.compute_energy_ssd_2d(delta_field)
return energy
def test_compute_residual_displacement_field_ssd_2d():
#Select arbitrary images' shape (same shape for both images)
sh = (20, 10)
#Select arbitrary centers
c_f = np.asarray(sh)/2
c_g = c_f + 0.5
#Compute the identity vector field I(x) = x in R^2
x_0 = np.asarray(range(sh[0]))
x_1 = np.asarray(range(sh[1]))
X = np.ndarray(sh + (2,), dtype = np.float64)
O = np.ones(sh)
X[...,0]= x_0[:, None] * O
X[...,1]= x_1[None, :] * O
#Compute the gradient fields of F and G
np.random.seed(5512751)
grad_F = X - c_f
grad_G = X - c_g
Fnoise = np.random.ranf(np.size(grad_F)).reshape(grad_F.shape) * grad_F.max() * 0.1
Fnoise = Fnoise.astype(floating)
grad_F += Fnoise
Gnoise = np.random.ranf(np.size(grad_G)).reshape(grad_G.shape) * grad_G.max() * 0.1
Gnoise = Gnoise.astype(floating)
grad_G += Gnoise
#The squared norm of grad_G
sq_norm_grad_G = np.sum(grad_G**2,-1)
#Compute F and G
F = 0.5*np.sum(grad_F**2,-1)
G = 0.5*sq_norm_grad_G
Fnoise = np.random.ranf(np.size(F)).reshape(F.shape) * F.max() * 0.1
Fnoise = Fnoise.astype(floating)
F += Fnoise
Gnoise = np.random.ranf(np.size(G)).reshape(G.shape) * G.max() * 0.1
Gnoise = Gnoise.astype(floating)
G += Gnoise
delta_field = np.array(F - G, dtype = floating)
sigma_field = np.random.randn(delta_field.size).reshape(delta_field.shape)
sigma_field = sigma_field.astype(floating)
#Select some pixels to force sigma_field = infinite
inf_sigma = np.random.randint(0, 2, sh[0]*sh[1])
inf_sigma = inf_sigma.reshape(sh)
sigma_field[inf_sigma == 1] = np.inf
#Select an initial displacement field
d = np.random.randn(grad_G.size).reshape(grad_G.shape).astype(floating)
#d = np.zeros_like(grad_G, dtype=floating)
lambda_param = 1.5
#Implementation under test
iut = ssd.compute_residual_displacement_field_ssd_2d
#In the first iteration we test the case target=None
#In the second iteration, target is not None
target = None
rtol = 1e-9
atol = 1e-4
for it in range(2):
# Sum of differences with the neighbors
s = np.zeros_like(d, dtype = np.float64)
s[:,:-1] += d[:,:-1] - d[:,1:]#right
s[:,1:] += d[:,1:] - d[:,:-1]#left
s[:-1,:] += d[:-1,:] - d[1:,:]#down
s[1:,:] += d[1:,:] - d[:-1,:]#up
s *= lambda_param
# Dot product of displacement and gradient
dp = d[...,0]*grad_G[...,0] + \
d[...,1]*grad_G[...,1]
dp = dp.astype(np.float64)
# Compute expected residual
expected = None
if target is None:
expected = np.zeros_like(grad_G)
expected[...,0] = delta_field*grad_G[...,0]
expected[...,1] = delta_field*grad_G[...,1]
else:
expected = target.copy().astype(np.float64)
# Expected residuals when sigma != infinte
expected[inf_sigma==0,0] -= grad_G[inf_sigma==0, 0] * dp[inf_sigma==0] + \
sigma_field[inf_sigma==0] * s[inf_sigma==0, 0]
expected[inf_sigma==0,1] -= grad_G[inf_sigma==0, 1] * dp[inf_sigma==0] + \
sigma_field[inf_sigma==0] * s[inf_sigma==0, 1]
# Expected residuals when sigma == infinte
expected[inf_sigma==1] = -1.0 * s[inf_sigma==1]
# Test residual field computation starting with residual = None
actual = iut(delta_field, sigma_field, grad_G.astype(floating),
target, lambda_param, d, None)
assert_allclose(actual, expected, rtol = rtol, atol = atol)
actual = np.ndarray(actual.shape, dtype=floating) #destroy previous result
# Test residual field computation starting with residual is not None
iut(delta_field, sigma_field, grad_G.astype(floating),
target, lambda_param, d, actual)
assert_allclose(actual, expected, rtol = rtol, atol = atol)
# Set target for next iteration
target = actual
# Test Gauss-Seidel step with residual=None and residual=target
for residual in [None, target]:
expected = d.copy()
iterate_residual_field_ssd_2d(delta_field, sigma_field,
grad_G.astype(floating), residual, lambda_param, expected)
actual = d.copy()
ssd.iterate_residual_displacement_field_ssd_2d(delta_field,
sigma_field, grad_G.astype(floating), residual, lambda_param, actual)
assert_allclose(actual, expected, rtol = rtol, atol = atol)
