def dp_vector_match_result():
res = np.empty(4, dtype="object")
res[0] = OrientationResult(0, euler2mat(*np.deg2rad([90, 0, 0]), 'rzxz'), 0.6, np.array([0.1, 0.10, 0.2]), 0.3, 1.0, 0, 0)
res[1] = OrientationResult(0, euler2mat(*np.deg2rad([0, 10, 20]), 'rzxz'), 0.5, np.array([0.1, 0.05, 0.2]), 0.4, 1.0, 0, 0)
res[2] = OrientationResult(1, euler2mat(*np.deg2rad([0, 45, 45]), 'rzxz'), 0.8, np.array([0.1, 0.30, 0.2]), 0.1, 1.0, 0, 0)
res[3] = OrientationResult(1, euler2mat(*np.deg2rad([0, 0, 90]), 'rzxz'), 0.7, np.array([0.1, 0.05, 0.1]), 0.2, 1.0, 0, 0)
return res
def sp_vector_match_result():
# We require (total_error of row_1 > correlation row_2)
res = np.empty(2, dtype="object")
res[0] = OrientationResult(0, euler2mat(*np.deg2rad([0, 0, 90]), 'rzxz'),
0.5, np.array([0.1, 0.05, 0.2]), 0.1, 1.0, 0, 0)
res[1] = OrientationResult(0, euler2mat(*np.deg2rad([0, 0, 90]), 'rzxz'),
0.6, np.array([0.1, 0.10, 0.2]), 0.2, 1.0, 0, 0)
return res
def dp_vector_match_result():
res = np.empty(4, dtype="object")
res = res.reshape(2,2)
res[0,0] = OrientationResult(
0,
euler2mat(*np.deg2rad([90, 0, 0]), "rzxz"),
0.6,
np.array([0.1, 0.10, 0.2]),
0.3,
1.0,
0,
0,
)
res[0,1] = OrientationResult(
0,
euler2mat(*np.deg2rad([0, 10, 20]), "rzxz"),
0.5,
np.array([0.1, 0.05, 0.2]),
0.4,
1.0,
0,
0,
)
res[1,0] = OrientationResult(
1,
euler2mat(*np.deg2rad([0, 45, 45]), "rzxz"),
0.8,
np.array([0.1, 0.30, 0.2]),
0.1,
1.0,
0,
0,
)
res[1,1] = OrientationResult(
1,
euler2mat(*np.deg2rad([0, 0, 90]), "rzxz"),
0.7,
np.array([0.1, 0.05, 0.1]),
0.2,
1.0,
0,
0,
)
return VectorMatchingResults(res)
def _refine_orientation(
solution,
k_xy,
structure_library,
accelarating_voltage,
camera_length,
index_error_tol=0.2,
method="leastsq",
vary_angles=True,
vary_center=False,
vary_scale=False,
verbose=False,
):
"""
Refine a single orientation agains the given cartesian vector coordinates.
Parameters
----------
solution : OrientationResult
Namedtuple containing the starting orientation
k_xy : DiffractionVectors
DiffractionVectors (x,y pixel format) to be indexed.
structure_library : :obj:`diffsims:StructureLibrary` Object
Dictionary of structures and associated orientations for which
electron diffraction is to be simulated.
index_error_tol : float
Max allowed error in peak indexation for classifying it as indexed,
calculated as :math:`|hkl_calculated - round(hkl_calculated)|`.
method : str
Minimization algorithm to use, choose from:
'leastsq', 'nelder', 'powell', 'cobyla', 'least-squares'.
See `lmfit` documentation (https://lmfit.github.io/lmfit-py/fitting.html)
for more information.
vary_angles : bool,
Free the euler angles (rotation matrix) during the refinement.
vary_center : bool
Free the center of the diffraction pattern (beam center) during the refinement.
vary_scale : bool
Free the scale (i.e. pixel size) of the diffraction vectors during refinement.
verbose : bool
Be more verbose
Returns
-------
result : OrientationResult
Container for the orientation refinement results
"""
# prepare reciprocal_lattice
structure = structure_library.structures[solution.phase_index]
lattice_recip = structure.lattice.reciprocal()
def objfunc(params, k_xy, lattice_recip, wavelength, camera_length):
cx = params["center_x"].value
cy = params["center_y"].value
ai = params["ai"].value
aj = params["aj"].value
ak = params["ak"].value
scale = params["scale"].value
rotmat = euler2mat(ai, aj, ak)
k_xy = k_xy + np.array((cx, cy)) * scale
cart = detector_to_fourier(k_xy, wavelength, camera_length)
intermediate = cart.dot(rotmat.T) # Must use the transpose here
hklss = lattice_recip.fractional(intermediate) * scale
rhklss = np.rint(hklss)
ehklss = np.abs(hklss - rhklss)
return ehklss
ai, aj, ak = mat2euler(solution.rotation_matrix)
params = lmfit.Parameters()
params.add("center_x", value=solution.center_x, vary=vary_center)
params.add("center_y", value=solution.center_y, vary=vary_center)
params.add("ai", value=ai, vary=vary_angles)
params.add("aj", value=aj, vary=vary_angles)
params.add("ak", value=ak, vary=vary_angles)
params.add("scale",
value=solution.scale,
vary=vary_scale,
min=0.8,
max=1.2)
wavelength = get_electron_wavelength(accelarating_voltage)
camera_length = camera_length * 1e10
args = k_xy, lattice_recip, wavelength, camera_length
res = lmfit.minimize(objfunc, params, args=args, method=method)
if verbose: # pragma: no cover
lmfit.report_fit(res)
p = res.params
ai, aj, ak = p["ai"].value, p["aj"].value, p["ak"].value
scale = p["scale"].value
center_x = params["center_x"].value
center_y = params["center_y"].value
rotation_matrix = euler2mat(ai, aj, ak)
k_xy = k_xy + np.array((center_x, center_y)) * scale
cart = detector_to_fourier(k_xy,
wavelength=wavelength,
camera_length=camera_length)
intermediate = cart.dot(rotation_matrix.T) # Must use the transpose here
hklss = lattice_recip.fractional(intermediate)
rhklss = np.rint(hklss)
error_hkls = res.residual.reshape(-1, 3)
error_mean = np.mean(error_hkls)
valid_peak_mask = np.max(error_hkls, axis=-1) < index_error_tol
valid_peak_count = np.count_nonzero(valid_peak_mask, axis=-1)
num_peaks = len(k_xy)
match_rate = (valid_peak_count * (1 / num_peaks)) if num_peaks else 0
orientation = OrientationResult(
phase_index=solution.phase_index,
rotation_matrix=rotation_matrix,
match_rate=match_rate,
error_hkls=error_hkls,
total_error=error_mean,
scale=scale,
center_x=center_x,
center_y=center_y,
)
res = np.empty(2, dtype=np.object)
res[0] = orientation
res[1] = rhklss
return res