def get_maxima(self, threshold=5.0):
'''Run diffdump, printpeaks to get a list of diffraction maxima
at their image positions, to allow for further analysis.'''
if not self._image:
raise RuntimeError('image not set')
if not os.path.exists(self._image):
raise RuntimeError('image %s does not exist' % \
self._image)
dd = Diffdump()
dd.set_image(self._image)
header = dd.readheader()
beam = header['raw_beam']
pixel = header['pixel']
template, directory = image2template_directory(self._image)
image_number = image2image(os.path.split(self._image)[-1])
spot_file = '%s.spt' % template_number2image(
template, image_number)
self.start()
self.input('template "%s"' % template)
self.input('directory "%s"' % directory)
self.input('findspots local find %d file %s' % \
(image_number, spot_file))
self.input('go')
self.close_wait()
self.check_for_errors()
output = open(os.path.join(self.get_working_directory(),
spot_file)).readlines()
os.remove(os.path.join(self.get_working_directory(), spot_file))
peaks = []
for record in output[3:-2]:
lst = record.split()
x = float(lst[0])
y = float(lst[1])
i = float(lst[4]) / float(lst[5])
x /= pixel[0]
y /= pixel[1]
if i < threshold:
continue
# this is Mosflm right? Swap X & Y!!
peaks.append((y, x, i))
return peaks
def epocher(images):
'''Get a list of epochs for each image in this list, returning as
a list of tuples.'''
result = []
for i in images:
dd = Diffdump()
dd.set_image(i)
header = dd.readheader()
e = header['epoch']
result.append((i, e))
return result
def epocher(images):
'''Get a list of epochs for each image in this list, returning as
a list of tuples.'''
result = []
for i in images:
dd = Diffdump()
dd.set_image(i)
header = dd.readheader()
e = header['epoch']
result.append((i, e))
return result
def _read_headers(self):
'''Get the image headers for all of the images - this is not designed
to be called externally.'''
self._headers = { }
t = time.time()
for i in self._images:
dd = Diffdump()
image = self.imagename(i)
dd.set_image(image)
header = dd.readheader()
self._headers[i] = header
return
def get_maxima(self):
'''Run diffdump, printpeaks to get a list of diffraction maxima
at their image positions, to allow for further analysis.'''
if not self._image:
raise RuntimeError('image not set')
if not os.path.exists(self._image):
raise RuntimeError('image %s does not exist' % \
self._image)
dd = Diffdump()
dd.set_image(self._image)
header = dd.readheader()
beam = header['raw_beam']
pixel = header['pixel']
self.add_command_line(self._image)
self.start()
self.close_wait()
self.check_for_errors()
# results were ok, so get all of the output out
output = self.get_all_output()
peaks = []
for record in output:
if not 'Peak' in record[:4]:
continue
lst = record.replace(':', ' ').split()
x = float(lst[4])
y = float(lst[6])
i = float(lst[-1])
x += beam[0]
y += beam[1]
x /= pixel[0]
y /= pixel[1]
peaks.append((x, y, i))
return peaks
def accumulate(images):
'''Accumulate dose as a function of image epoch.'''
dose = { }
integrated_dose = { }
for i in images:
dd = Diffdump()
dd.set_image(i)
header = dd.readheader()
d = header['exposure_time']
e = header['epoch']
dose[e] = d
keys = dose.keys()
keys.sort()
accum = 0.0
for k in keys:
integrated_dose[k] = accum + 0.5 * dose[k]
accum += dose[k]
# ok, now check that the value for the maximum dose is < 1e6 - elsewise
# chef may explode. or write out ****** as the values are too large for
# an f8.1 format statement.
max_dose = max([integrated_dose[k] for k in keys])
factor = 1.0
while max_dose / factor > 1.0e6:
factor *= 10.0
Debug.write('Doses scaled by %5.2e' % factor)
# now divide all of those doses by factor
for k in keys:
integrated_dose[k] /= factor
return integrated_dose, factor
def test_i(self):
idxref = self.Idxref()
self._index_remove_masked_regions()
for file in ['SPOT.XDS']:
idxref.set_input_data_file(file, self._indxr_payload[file])
idxref.set_data_range(self._indxr_images[0][0],
self._indxr_images[0][1])
idxref.set_background_range(self._indxr_images[0][0],
self._indxr_images[0][1])
# set the phi start etc correctly
blocks = self._index_select_images_i()
for block in blocks[:1]:
starting_frame = block[0]
dd = Diffdump()
dd.set_image(self.get_image_name(starting_frame))
starting_angle = dd.readheader()['phi_start']
idxref.set_starting_frame(starting_frame)
idxref.set_starting_angle(starting_angle)
idxref.add_spot_range(block[0], block[1])
for block in blocks[1:]:
idxref.add_spot_range(block[0], block[1])
#mosflm_beam_centre = self.get_beam_centre()
#xds_beam_centre = beam_centre_mosflm_to_xds(
#mosflm_beam_centre[0], mosflm_beam_centre[1], self.get_header())
from dxtbx.serialize.xds import to_xds
converter = to_xds(self.get_imageset())
xds_beam_centre = converter.detector_origin
idxref.set_beam_centre(xds_beam_centre[0],
xds_beam_centre[1])
idxref.run()
return idxref.get_fraction_rmsd_rmsphi()
def accumulate(images):
'''Accumulate dose as a function of image epoch.'''
dose = {}
integrated_dose = {}
for i in images:
dd = Diffdump()
dd.set_image(i)
header = dd.readheader()
d = header['exposure_time']
e = header['epoch']
dose[e] = d
keys = sorted(dose.keys())
accum = 0.0
for k in keys:
integrated_dose[k] = accum + 0.5 * dose[k]
accum += dose[k]
# ok, now check that the value for the maximum dose is < 1e6 - elsewise
# chef may explode. or write out ****** as the values are too large for
# an f8.1 format statement.
max_dose = max([integrated_dose[k] for k in keys])
factor = 1.0
while max_dose / factor > 1.0e6:
factor *= 10.0
Debug.write('Doses scaled by %5.2e' % factor)
# now divide all of those doses by factor
for k in keys:
integrated_dose[k] /= factor
return integrated_dose, factor
assert 0.0 <= i[0] <= 2.0
assert 0.0 <= i[1] <= 2.0
assert math.fabs((dot(x, d) / math.sqrt(dot(x, x) * dot(d, d))) -
1) < 0.001
if __name__ == "__main_work__":
work_equation_of_line()
if __name__ == "__main__":
from xia2.Wrappers.XIA.Diffdump import Diffdump
bm = BackstopMask(sys.argv[1])
dd = Diffdump()
dd.set_image(sys.argv[2])
header = dd.readheader()
def format_limits(limits):
assert len(limits) == 4
result = "limits quad"
for l in limits:
result += " %.1f %.1f" % l
return result
print(format_limits(bm.calculate_mask_mosflm(header)))
def gain(image):
"""Get the gain from an image."""
dd = Diffdump()
dd.set_image(image)
return dd.gain()
assert 0.0 <= i[1] <= 2.0
assert math.fabs((dot(x, d) / math.sqrt(dot(x, x) * dot(d, d))) - 1) < 0.001
return
if __name__ == "__main_work__":
work_equation_of_line()
if __name__ == "__main__":
from xia2.Wrappers.XIA.Diffdump import Diffdump
bm = BackstopMask(sys.argv[1])
dd = Diffdump()
dd.set_image(sys.argv[2])
header = dd.readheader()
def format_limits(limits):
assert len(limits) == 4
result = "limits quad"
for l in limits:
result += " %.1f %.1f" % l
return result
print format_limits(bm.calculate_mask_mosflm(header))
def mosflm_check_indexer_solution(indexer):
distance = indexer.get_indexer_distance()
axis = matrix.col([0, 0, 1])
beam = indexer.get_indexer_beam_centre()
cell = indexer.get_indexer_cell()
wavelength = indexer.get_wavelength()
space_group_number = l2s(indexer.get_indexer_lattice())
spacegroup = sgtbx.space_group_symbols(space_group_number).hall()
phi = indexer.get_header()['phi_width']
sg = sgtbx.space_group(spacegroup)
if not (sg.n_ltr() - 1):
# primitive solution - just return ... something
return None, None, None, None
# FIXME need to raise an exception if this is not available!
m_matrix = indexer.get_indexer_payload('mosflm_orientation_matrix')
# N.B. in the calculation below I am using the Cambridge frame
# and Mosflm definitions of X & Y...
m_elems = []
for record in m_matrix[:3]:
record = record.replace('-', ' -')
for e in map(float, record.split()):
m_elems.append(e / wavelength)
mi = matrix.sqr(m_elems)
m = mi.inverse()
A = matrix.col(m.elems[0:3])
B = matrix.col(m.elems[3:6])
C = matrix.col(m.elems[6:9])
# now select the images - start with the images that the indexer
# used for indexing, though can interrogate the FrameProcessor
# interface of the indexer to put together a completely different
# list if I like...
images = []
for i in indexer.get_indexer_images():
for j in i:
if not j in images:
images.append(j)
images.sort()
# now construct the reciprocal-space peak list n.b. should
# really run this in parallel...
spots_r = []
spots_r_j = { }
for i in images:
image = indexer.get_image_name(i)
dd = Diffdump()
dd.set_image(image)
header = dd.readheader()
phi = header['phi_start'] + 0.5 * header['phi_width']
pixel = header['pixel']
wavelength = header['wavelength']
peaks = locate_maxima(image)
spots_r_j[i] = []
for p in peaks:
x, y, isigma = p
if isigma < 5.0:
continue
xp = pixel[0] * y - beam[0]
yp = pixel[1] * x - beam[1]
scale = wavelength * math.sqrt(
xp * xp + yp * yp + distance * distance)
X = distance / scale
X -= 1.0 / wavelength
Y = - xp / scale
Z = yp / scale
S = matrix.col([X, Y, Z])
rtod = 180.0 / math.pi
spots_r.append(S.rotate(axis, - phi / rtod))
spots_r_j[i].append(S.rotate(axis, - phi / rtod))
# now reindex the reciprocal space spot list and count - n.b. need
# to transform the Bravais lattice to an assumed spacegroup and hence
# to a cctbx spacegroup!
# lists = [spots_r_j[j] for j in spots_r_j]
lists = []
lists.append(spots_r)
for l in lists:
absent = 0
present = 0
total = 0
for spot in l:
hkl = (m * spot).elems
total += 1
ihkl = map(nint, hkl)
if math.fabs(hkl[0] - ihkl[0]) > 0.1:
continue
if math.fabs(hkl[1] - ihkl[1]) > 0.1:
continue
if math.fabs(hkl[2] - ihkl[2]) > 0.1:
continue
# now determine if it is absent
if sg.is_sys_absent(ihkl):
absent += 1
else:
present += 1
# now perform the analysis on these numbers...
sd = math.sqrt(absent)
if total:
Debug.write('Counts: %d %d %d %.3f' % \
(total, present, absent, (absent - 3 * sd) / total))
else:
Debug.write('Not enough spots found for analysis')
return False, None, None, None
if (absent - 3 * sd) / total < 0.008:
return False, None, None, None
# in here need to calculate the new orientation matrix for the
# primitive basis and reconfigure the indexer - somehow...
# ok, so the bases are fine, but what I will want to do is reorder them
# to give the best primitive choice of unit cell...
sgp = sg.build_derived_group(True, False)
lattice_p = s2l(sgp.type().number())
symm = crystal.symmetry(unit_cell = cell,
space_group = sgp)
rdx = symm.change_of_basis_op_to_best_cell()
symm_new = symm.change_basis(rdx)
# now apply this to the reciprocal-space orientation matrix mi
# cb_op = sgtbx.change_of_basis_op(rdx)
cb_op = rdx
R = cb_op.c_inv().r().as_rational().as_float().transpose().inverse()
mi_r = mi * R
# now re-derive the cell constants, just to be sure
m_r = mi_r.inverse()
Ar = matrix.col(m_r.elems[0:3])
Br = matrix.col(m_r.elems[3:6])
Cr = matrix.col(m_r.elems[6:9])
a = math.sqrt(Ar.dot())
b = math.sqrt(Br.dot())
c = math.sqrt(Cr.dot())
rtod = 180.0 / math.pi
alpha = rtod * Br.angle(Cr)
beta = rtod * Cr.angle(Ar)
gamma = rtod * Ar.angle(Br)
# print '%6.3f %6.3f %6.3f %6.3f %6.3f %6.3f' % \
# (a, b, c, alpha, beta, gamma)
cell = uctbx.unit_cell((a, b, c, alpha, beta, gamma))
amat = [wavelength * e for e in mi_r.elems]
bmat = matrix.sqr(cell.fractionalization_matrix())
umat = mi_r * bmat.inverse()
# yuk! surely I don't need to do this...
# I do need to do this, and don't call me shirley!
new_matrix = ['%s\n' % r for r in \
format_matrix((a, b, c, alpha, beta, gamma),
amat, umat.elems).split('\n')]
# ok - this gives back the right matrix in the right setting - excellent!
# now need to apply this back at base to the results of the indexer.
# N.B. same should be applied to the same calculations for the XDS
# version of this.
return True, lattice_p, new_matrix, (a, b, c, alpha, beta, gamma)
def mosflm_check_indexer_solution(indexer):
distance = indexer.get_indexer_distance()
axis = matrix.col([0, 0, 1])
beam = indexer.get_indexer_beam_centre()
cell = indexer.get_indexer_cell()
wavelength = indexer.get_wavelength()
space_group_number = l2s(indexer.get_indexer_lattice())
spacegroup = sgtbx.space_group_symbols(space_group_number).hall()
phi = indexer.get_header()['phi_width']
sg = sgtbx.space_group(spacegroup)
if not (sg.n_ltr() - 1):
# primitive solution - just return ... something
return None, None, None, None
# FIXME need to raise an exception if this is not available!
m_matrix = indexer.get_indexer_payload('mosflm_orientation_matrix')
# N.B. in the calculation below I am using the Cambridge frame
# and Mosflm definitions of X & Y...
m_elems = []
for record in m_matrix[:3]:
record = record.replace('-', ' -')
for e in map(float, record.split()):
m_elems.append(e / wavelength)
mi = matrix.sqr(m_elems)
m = mi.inverse()
A = matrix.col(m.elems[0:3])
B = matrix.col(m.elems[3:6])
C = matrix.col(m.elems[6:9])
# now select the images - start with the images that the indexer
# used for indexing, though can interrogate the FrameProcessor
# interface of the indexer to put together a completely different
# list if I like...
images = []
for i in indexer.get_indexer_images():
for j in i:
if not j in images:
images.append(j)
images.sort()
# now construct the reciprocal-space peak list n.b. should
# really run this in parallel...
spots_r = []
spots_r_j = {}
for i in images:
image = indexer.get_image_name(i)
dd = Diffdump()
dd.set_image(image)
header = dd.readheader()
phi = header['phi_start'] + 0.5 * header['phi_width']
pixel = header['pixel']
wavelength = header['wavelength']
peaks = locate_maxima(image)
spots_r_j[i] = []
for p in peaks:
x, y, isigma = p
if isigma < 5.0:
continue
xp = pixel[0] * y - beam[0]
yp = pixel[1] * x - beam[1]
scale = wavelength * math.sqrt(xp * xp + yp * yp +
distance * distance)
X = distance / scale
X -= 1.0 / wavelength
Y = -xp / scale
Z = yp / scale
S = matrix.col([X, Y, Z])
rtod = 180.0 / math.pi
spots_r.append(S.rotate(axis, -phi / rtod))
spots_r_j[i].append(S.rotate(axis, -phi / rtod))
# now reindex the reciprocal space spot list and count - n.b. need
# to transform the Bravais lattice to an assumed spacegroup and hence
# to a cctbx spacegroup!
# lists = [spots_r_j[j] for j in spots_r_j]
lists = []
lists.append(spots_r)
for l in lists:
absent = 0
present = 0
total = 0
for spot in l:
hkl = (m * spot).elems
total += 1
ihkl = map(nint, hkl)
if math.fabs(hkl[0] - ihkl[0]) > 0.1:
continue
if math.fabs(hkl[1] - ihkl[1]) > 0.1:
continue
if math.fabs(hkl[2] - ihkl[2]) > 0.1:
continue
# now determine if it is absent
if sg.is_sys_absent(ihkl):
absent += 1
else:
present += 1
# now perform the analysis on these numbers...
sd = math.sqrt(absent)
if total:
Debug.write('Counts: %d %d %d %.3f' % \
(total, present, absent, (absent - 3 * sd) / total))
else:
Debug.write('Not enough spots found for analysis')
return False, None, None, None
if (absent - 3 * sd) / total < 0.008:
return False, None, None, None
# in here need to calculate the new orientation matrix for the
# primitive basis and reconfigure the indexer - somehow...
# ok, so the bases are fine, but what I will want to do is reorder them
# to give the best primitive choice of unit cell...
sgp = sg.build_derived_group(True, False)
lattice_p = s2l(sgp.type().number())
symm = crystal.symmetry(unit_cell=cell, space_group=sgp)
rdx = symm.change_of_basis_op_to_best_cell()
symm_new = symm.change_basis(rdx)
# now apply this to the reciprocal-space orientation matrix mi
# cb_op = sgtbx.change_of_basis_op(rdx)
cb_op = rdx
R = cb_op.c_inv().r().as_rational().as_float().transpose().inverse()
mi_r = mi * R
# now re-derive the cell constants, just to be sure
m_r = mi_r.inverse()
Ar = matrix.col(m_r.elems[0:3])
Br = matrix.col(m_r.elems[3:6])
Cr = matrix.col(m_r.elems[6:9])
a = math.sqrt(Ar.dot())
b = math.sqrt(Br.dot())
c = math.sqrt(Cr.dot())
rtod = 180.0 / math.pi
alpha = rtod * Br.angle(Cr)
beta = rtod * Cr.angle(Ar)
gamma = rtod * Ar.angle(Br)
# print '%6.3f %6.3f %6.3f %6.3f %6.3f %6.3f' % \
# (a, b, c, alpha, beta, gamma)
cell = uctbx.unit_cell((a, b, c, alpha, beta, gamma))
amat = [wavelength * e for e in mi_r.elems]
bmat = matrix.sqr(cell.fractionalization_matrix())
umat = mi_r * bmat.inverse()
# yuk! surely I don't need to do this...
# I do need to do this, and don't call me shirley!
new_matrix = ['%s\n' % r for r in \
format_matrix((a, b, c, alpha, beta, gamma),
amat, umat.elems).split('\n')]
# ok - this gives back the right matrix in the right setting - excellent!
# now need to apply this back at base to the results of the indexer.
# N.B. same should be applied to the same calculations for the XDS
# version of this.
return True, lattice_p, new_matrix, (a, b, c, alpha, beta, gamma)
def gain(image): '''Get the gain from an image.''' dd = Diffdump() dd.set_image(image) return dd.gain()
def gain(image):
'''Get the gain from an image.'''
dd = Diffdump()
dd.set_image(image)
return dd.gain()
def _index(self):
'''Actually do the autoindexing using the data prepared by the
previous method.'''
images_str = '%d to %d' % tuple(self._indxr_images[0])
for i in self._indxr_images[1:]:
images_str += ', %d to %d' % tuple(i)
cell_str = None
if self._indxr_input_cell:
cell_str = '%.2f %.2f %.2f %.2f %.2f %.2f' % \
self._indxr_input_cell
# then this is a proper autoindexing run - describe this
# to the journal entry
#if len(self._fp_directory) <= 50:
#dirname = self._fp_directory
#else:
#dirname = '...%s' % self._fp_directory[-46:]
dirname = self.get_directory()
Journal.block('autoindexing', self._indxr_sweep_name, 'XDS',
{'images':images_str,
'target cell':cell_str,
'target lattice':self._indxr_input_lattice,
'template':self.get_template(),
'directory':dirname})
idxref = self.Idxref()
self._index_remove_masked_regions()
for file in ['SPOT.XDS']:
idxref.set_input_data_file(file, self._indxr_payload[file])
idxref.set_data_range(self._indxr_images[0][0],
self._indxr_images[0][1])
idxref.set_background_range(self._indxr_images[0][0],
self._indxr_images[0][1])
# set the phi start etc correctly
if self._i_or_ii == None:
self._i_or_ii = self.decide_i_or_ii()
Debug.write('Selecting I or II, chose %s' % self._i_or_ii)
if self._i_or_ii == 'i':
blocks = self._index_select_images_i()
for block in blocks[:1]:
starting_frame = block[0]
dd = Diffdump()
dd.set_image(self.get_image_name(starting_frame))
starting_angle = dd.readheader()['phi_start']
idxref.set_starting_frame(starting_frame)
idxref.set_starting_angle(starting_angle)
idxref.add_spot_range(block[0], block[1])
for block in blocks[1:]:
idxref.add_spot_range(block[0], block[1])
else:
for block in self._indxr_images[:1]:
starting_frame = block[0]
dd = Diffdump()
dd.set_image(self.get_image_name(starting_frame))
starting_angle = dd.readheader()['phi_start']
idxref.set_starting_frame(starting_frame)
idxref.set_starting_angle(starting_angle)
idxref.add_spot_range(block[0], block[1])
for block in self._indxr_images[1:]:
idxref.add_spot_range(block[0], block[1])
# FIXME need to also be able to pass in the known unit
# cell and lattice if already available e.g. from
# the helper... indirectly
if self._indxr_user_input_lattice:
idxref.set_indexer_user_input_lattice(True)
if self._indxr_input_lattice and self._indxr_input_cell:
idxref.set_indexer_input_lattice(self._indxr_input_lattice)
idxref.set_indexer_input_cell(self._indxr_input_cell)
Debug.write('Set lattice: %s' % self._indxr_input_lattice)
Debug.write('Set cell: %f %f %f %f %f %f' % \
self._indxr_input_cell)
original_cell = self._indxr_input_cell
elif self._indxr_input_lattice:
idxref.set_indexer_input_lattice(self._indxr_input_lattice)
original_cell = None
else:
original_cell = None
# FIXED need to set the beam centre here - this needs to come
# from the input .xinfo object or header, and be converted
# to the XDS frame... done.
#mosflm_beam_centre = self.get_beam_centre()
#xds_beam_centre = beam_centre_mosflm_to_xds(
#mosflm_beam_centre[0], mosflm_beam_centre[1], self.get_header())
from dxtbx.serialize.xds import to_xds
converter = to_xds(self.get_imageset())
xds_beam_centre = converter.detector_origin
idxref.set_beam_centre(xds_beam_centre[0],
xds_beam_centre[1])
# fixme need to check if the lattice, cell have been set already,
# and if they have, pass these in as input to the indexing job.
done = False
while not done:
try:
done = idxref.run()
# N.B. in here if the IDXREF step was being run in the first
# pass done is FALSE however there should be a refined
# P1 orientation matrix etc. available - so keep it!
except XDSException, e:
# inspect this - if we have complaints about not
# enough reflections indexed, and we have a target
# unit cell, and they are the same, well ignore it
if 'solution is inaccurate' in str(e):
Debug.write(
'XDS complains solution inaccurate - ignoring')
done = idxref.continue_from_error()
elif ('insufficient percentage (< 70%)' in str(e) or
'insufficient percentage (< 50%)' in str(e)) and \
original_cell:
done = idxref.continue_from_error()
lattice, cell, mosaic = \
idxref.get_indexing_solution()
# compare solutions
for j in range(3):
# allow two percent variation in unit cell length
if math.fabs((cell[j] - original_cell[j]) / \
original_cell[j]) > 0.02 and \
not Flags.get_relax():
Debug.write('XDS unhappy and solution wrong')
raise e
# and two degree difference in angle
if math.fabs(cell[j + 3] - original_cell[j + 3]) \
> 2.0 and not Flags.get_relax():
Debug.write('XDS unhappy and solution wrong')
raise e
Debug.write('XDS unhappy but solution ok')
elif 'insufficient percentage (< 70%)' in str(e) or \
'insufficient percentage (< 50%)' in str(e):
Debug.write('XDS unhappy but solution probably ok')
done = idxref.continue_from_error()
else:
raise e
