def get_map_values_and_grid_sites_frac(fmodel, map_type, grid_step, d_min,
apply_sigma_scaling,
apply_volume_scaling, include_f000,
sel_bb, use_exact_phases):
#
resolution_factor = grid_step / d_min
mp = mmtbx.masks.mask_master_params.extract()
mp.grid_step_factor = 1. / resolution_factor
mmtbx_masks_asu_mask_obj = mmtbx.masks.asu_mask(
xray_structure=fmodel.xray_structure, d_min=d_min, mask_params=mp)
bulk_solvent_mask = mmtbx_masks_asu_mask_obj.mask_data_whole_uc()
sel = bulk_solvent_mask > 0
bulk_solvent_mask = bulk_solvent_mask.set_selected(sel, 1)
cr_gr = maptbx.crystal_gridding(
unit_cell=fmodel.xray_structure.unit_cell(),
space_group_info=fmodel.f_obs().space_group_info(),
pre_determined_n_real=bulk_solvent_mask.focus())
from mmtbx import map_tools
from cctbx import miller
#
#mc = map_tools.electron_density_map(fmodel = fmodel).map_coefficients(
# map_type = map_type,
# acentrics_scale = 1.0,
# centrics_pre_scale = 1.0)
if not use_exact_phases:
k = fmodel.k_isotropic() * fmodel.k_anisotropic()
print("flex.mean(k):", flex.mean(k))
f_model = fmodel.f_model()
mc_data = abs(fmodel.f_obs()).data() / k - abs(f_model).data() / k
tmp = miller.array(miller_set=f_model,
data=flex.double(
f_model.indices().size(),
1)).phase_transfer(phase_source=f_model)
mc = miller.array(miller_set=tmp, data=mc_data * tmp.data())
else:
fmodel.update_all_scales(fast=True, remove_outliers=False)
k = fmodel.k_isotropic() * fmodel.k_anisotropic()
fo = fmodel.f_obs().customized_copy(data=fmodel.f_obs().data() / k)
fo = fo.phase_transfer(phase_source=fmodel.f_model())
fc = fmodel.f_calc().customized_copy(data=fmodel.f_calc().data())
mc = miller.array(miller_set=fo, data=fo.data() - fc.data())
######## XXX
fft_map = miller.fft_map(crystal_gridding=cr_gr, fourier_coefficients=mc)
fft_map.apply_volume_scaling()
map_data = fft_map.real_map_unpadded()
xrs = fmodel.xray_structure
sites_cart = xrs.sites_cart().select(sel_bb)
sel = maptbx.grid_indices_around_sites(unit_cell=xrs.unit_cell(),
fft_n_real=map_data.focus(),
fft_m_real=map_data.all(),
sites_cart=sites_cart,
site_radii=flex.double(
sites_cart.size(), 0.5))
map_in = map_data.select(sel)
mm = flex.mean(map_in)
print("mean in (1):", mm)
#
#sites_frac = xrs.sites_frac().select(sel_bb)
#mm = 0
#for sf in sites_frac:
# mm += map_data.eight_point_interpolation(sf)
#mm = mm/sites_frac.size()
#print "mean in (2):", mm
########
#
# Add F000
#reg = fmodel.xray_structure.scattering_type_registry(table = "wk1995")
#f_000 = reg.sum_of_scattering_factors_at_diffraction_angle_0() +\
# 0.4*fmodel.xray_structure.unit_cell().volume()
if (include_f000):
#f_000 = include_f000*fmodel.xray_structure.unit_cell().volume()*0.3
#f_000 = None # XXX
f_000 = abs(mm * xrs.unit_cell().volume())
#f_000 = 0.626*fmodel.xray_structure.unit_cell().volume()*0.35
else:
f_000 = None
print("f_000:", f_000)
#print "XXX", include_f000*fmodel.xray_structure.unit_cell().volume()*0.3
#
fft_map = miller.fft_map(crystal_gridding=cr_gr,
fourier_coefficients=mc,
f_000=f_000)
#
assert [apply_sigma_scaling, apply_volume_scaling].count(True) == 1
if (apply_sigma_scaling): fft_map.apply_sigma_scaling()
elif (apply_volume_scaling): fft_map.apply_volume_scaling()
else: assert RuntimeError
nx, ny, nz = fft_map.n_real()
map_data = fft_map.real_map_unpadded()
#map_data = map_data * bulk_solvent_mask
print("n_real:", nx, ny, nz, map_data.size())
grid_sites_frac = flex.vec3_double()
map_values = flex.double()
for ix in range(nx):
for iy in range(ny):
for iz in range(nz):
mv = map_data[(ix, iy, iz)]
if 1: #if(mv != 0):
xf, yf, zf = ix / float(nx), iy / float(ny), iz / float(nz)
grid_sites_frac.append([xf, yf, zf])
map_at_ixiyiz = map_data[(ix, iy, iz)]
map_values.append(map_at_ixiyiz)
return map_values, grid_sites_frac
def __init__ (self,
data_arrays,
xray_structure,
log=None,
silent=False,
output_file=None,
peak_search=False,
map_cutoff=None,
peak_search_params=None,
r_free_arrays=None,
write_map=True,
multiscale=False,
anomalous=False) :
if (log is None) : log = sys.stdout
adopt_init_args(self, locals())
fmodels = []
for i_seq, d in enumerate(data_arrays):
if(not silent):
print >> log, "Data set: %d"%i_seq
if(d.anomalous_flag()) and (not anomalous) :
d = d.average_bijvoet_mates()
elif (anomalous) :
assert d.anomalous_flag()
if (r_free_arrays is not None) and (i_seq < len(r_free_arrays)) :
r_free_flags = r_free_arrays[i_seq]
else :
r_free_flags = d.array(data = flex.bool(d.data().size(), False))
fmodel = mmtbx.f_model.manager(
xray_structure = xray_structure,
r_free_flags = r_free_flags,
target_name = "ls_wunit_k1",
f_obs = d)
fmodel.update_all_scales(log=None)
if(not silent):
fmodel.info().show_rfactors_targets_scales_overall(out=log)
print >> log
fmodels.append(fmodel)
self.fmodel = fmodels[0]
# prepare Fobs for map calculation (apply scaling):
f_obss = []
for fmodel in fmodels:
obs = fmodel.f_obs()
f_obs_scale = 1.0 / fmodel.k_anisotropic() / fmodel.k_isotropic()
obs = miller.array(miller_set = fmodel.f_model(),
data = obs.data()*f_obs_scale)
f_obss.append(obs)
# given two Fobs sets, make them one-to-one matching, get phases and map coefficients
# Note: f_calc below is just f_calc from atoms (no bulk solvent etc applied)
fobs_1, f_model = f_obss[0].common_sets(other = fmodels[1].f_model())
fobs_1, fobs_2 = fobs_1.common_sets(other = f_obss[1])
fobs_1, f_model = fobs_1.common_sets(other = f_model)
self.f_model = f_model
assert fobs_2.indices().all_eq(fobs_1.indices())
assert f_model.indices().all_eq(fobs_1.indices())
# scale again
scale_k1 = 1
den = flex.sum(flex.abs(fobs_2.data())*flex.abs(fobs_2.data()))
if(den != 0):
scale_k1 = flex.sum(flex.abs(fobs_1.data())*flex.abs(fobs_2.data())) / den
#
fobs_2 = fobs_2.array(data = fobs_2.data()*scale_k1)
if multiscale:
fobs_1 = fobs_2.multiscale(other = fobs_1, reflections_per_bin=250)
if(not silent):
print >> log, ""
print >> log, "Fobs1_vs_Fobs2 statistics:"
print >> log, "Bin# Resolution range Compl. No.of refl. CC R-factor"
fobs_1.setup_binner(reflections_per_bin = min(500, fobs_1.data().size()))
fobs_2.use_binning_of(fobs_1)
for i_bin in fobs_1.binner().range_used():
sel = fobs_1.binner().selection(i_bin)
f1 = fobs_1.select(sel)
f2 = fobs_2.select(sel)
d_max, d_min = fobs_1.d_max_min()
compl = fobs_1.completeness(d_max = d_max)
n_ref = sel.count(True)
num = flex.sum(flex.abs(f1.data()-f2.data()))
den = flex.sum(flex.abs(f1.data()+f2.data())/2)
r = None
if(den!=0):
r = num/den
cc = flex.linear_correlation(x=f1.data(), y=f2.data()).coefficient()
d_range = fobs_1.binner().bin_legend(
i_bin = i_bin, show_bin_number = False, show_counts = False)
fmt = "%3d: %-17s %4.2f %6d %5.3f %6s"
print >> log, fmt % (i_bin, d_range, compl, n_ref, cc,
format_value("%6.4f", r))
# overall statistics
self.cc = flex.linear_correlation(
x=fobs_1.data(),
y=fobs_2.data()).coefficient()
num = flex.sum(flex.abs(fobs_1.data()-fobs_2.data()))
den = flex.sum(flex.abs(fobs_2.data()+fobs_2.data())/2)
self.r_factor = None
if (den != 0) :
self.r_factor = num / den
# map coefficients
def phase_transfer(miller_array, phase_source):
tmp = miller.array(miller_set = miller_array,
data = flex.double(miller_array.indices().size(), 1)
).phase_transfer(phase_source = phase_source)
return miller.array(miller_set = miller_array,
data = miller_array.data() * tmp.data() )
if (not anomalous) :
diff = miller.array(
miller_set = f_model,
data = fobs_1.data()-fobs_2.data())
self.map_coeff = phase_transfer(
miller_array = diff,
phase_source = f_model)
else :
dano_1 = fobs_1.anomalous_differences()
dano_2 = fobs_2.anomalous_differences()
assert dano_1.indices().all_eq(dano_2.indices())
diff = miller.array(
miller_set = dano_1,
data = dano_1.data() - dano_2.data())
f_model_phases = f_model.average_bijvoet_mates().common_set(diff)
map_coeffs = phase_transfer(
miller_array = diff,
phase_source = f_model_phases)
self.map_coeff = map_coeffs.customized_copy(data=map_coeffs.data()/(2j))
if(self.map_coeff.anomalous_flag()):
self.map_coeff = map_coeff.average_bijvoet_mates()
self.file_names = []
if (write_map) :
self.file_names = self.write_map_file()
def __init__(self,
data_arrays,
xray_structure,
log=None,
silent=False,
output_file=None,
peak_search=False,
map_cutoff=None,
peak_search_params=None,
r_free_arrays=None,
write_map=True,
multiscale=False,
anomalous=False):
if (log is None): log = sys.stdout
adopt_init_args(self, locals())
fmodels = []
for i_seq, d in enumerate(data_arrays):
if (not silent):
print("Data set: %d" % i_seq, file=log)
if (d.anomalous_flag()) and (not anomalous):
d = d.average_bijvoet_mates()
elif (anomalous):
assert d.anomalous_flag()
if (r_free_arrays is not None) and (i_seq < len(r_free_arrays)):
r_free_flags = r_free_arrays[i_seq]
else:
r_free_flags = d.array(data=flex.bool(d.data().size(), False))
fmodel = mmtbx.f_model.manager(xray_structure=xray_structure,
r_free_flags=r_free_flags,
target_name="ls_wunit_k1",
f_obs=d)
fmodel.update_all_scales(log=None)
if (not silent):
fmodel.info().show_rfactors_targets_scales_overall(out=log)
print(file=log)
fmodels.append(fmodel)
self.fmodel = fmodels[0]
# prepare Fobs for map calculation (apply scaling):
f_obss = []
for fmodel in fmodels:
obs = fmodel.f_obs()
f_obs_scale = 1.0 / fmodel.k_anisotropic() / fmodel.k_isotropic()
obs = miller.array(miller_set=fmodel.f_model(),
data=obs.data() * f_obs_scale)
f_obss.append(obs)
# given two Fobs sets, make them one-to-one matching, get phases and map coefficients
# Note: f_calc below is just f_calc from atoms (no bulk solvent etc applied)
fobs_1, f_model = f_obss[0].common_sets(other=fmodels[1].f_model())
fobs_1, fobs_2 = fobs_1.common_sets(other=f_obss[1])
fobs_1, f_model = fobs_1.common_sets(other=f_model)
self.f_model = f_model
assert fobs_2.indices().all_eq(fobs_1.indices())
assert f_model.indices().all_eq(fobs_1.indices())
# scale again
scale_k1 = 1
den = flex.sum(flex.abs(fobs_2.data()) * flex.abs(fobs_2.data()))
if (den != 0):
scale_k1 = flex.sum(
flex.abs(fobs_1.data()) * flex.abs(fobs_2.data())) / den
#
fobs_2 = fobs_2.array(data=fobs_2.data() * scale_k1)
if multiscale:
fobs_1 = fobs_2.multiscale(other=fobs_1, reflections_per_bin=250)
if (not silent):
print("", file=log)
print("Fobs1_vs_Fobs2 statistics:", file=log)
print("Bin# Resolution range Compl. No.of refl. CC R-factor",
file=log)
fobs_1.setup_binner(
reflections_per_bin=min(500,
fobs_1.data().size()))
fobs_2.use_binning_of(fobs_1)
for i_bin in fobs_1.binner().range_used():
sel = fobs_1.binner().selection(i_bin)
f1 = fobs_1.select(sel)
f2 = fobs_2.select(sel)
d_max, d_min = fobs_1.d_max_min()
compl = fobs_1.completeness(d_max=d_max)
n_ref = sel.count(True)
num = flex.sum(flex.abs(f1.data() - f2.data()))
den = flex.sum(flex.abs(f1.data() + f2.data()) / 2)
r = None
if (den != 0):
r = num / den
cc = flex.linear_correlation(x=f1.data(),
y=f2.data()).coefficient()
d_range = fobs_1.binner().bin_legend(i_bin=i_bin,
show_bin_number=False,
show_counts=False)
fmt = "%3d: %-17s %4.2f %6d %5.3f %6s"
print(fmt % (i_bin, d_range, compl, n_ref, cc,
format_value("%6.4f", r)),
file=log)
# overall statistics
self.cc = flex.linear_correlation(x=fobs_1.data(),
y=fobs_2.data()).coefficient()
num = flex.sum(flex.abs(fobs_1.data() - fobs_2.data()))
den = flex.sum(flex.abs(fobs_2.data() + fobs_2.data()) / 2)
self.r_factor = None
if (den != 0):
self.r_factor = num / den
# map coefficients
def phase_transfer(miller_array, phase_source):
tmp = miller.array(
miller_set=miller_array,
data=flex.double(miller_array.indices().size(),
1)).phase_transfer(phase_source=phase_source)
return miller.array(miller_set=miller_array,
data=miller_array.data() * tmp.data())
if (not anomalous):
diff = miller.array(miller_set=f_model,
data=fobs_1.data() - fobs_2.data())
self.map_coeff = phase_transfer(miller_array=diff,
phase_source=f_model)
else:
dano_1 = fobs_1.anomalous_differences()
dano_2 = fobs_2.anomalous_differences()
assert dano_1.indices().all_eq(dano_2.indices())
diff = miller.array(miller_set=dano_1,
data=dano_1.data() - dano_2.data())
f_model_phases = f_model.average_bijvoet_mates().common_set(diff)
map_coeffs = phase_transfer(miller_array=diff,
phase_source=f_model_phases)
self.map_coeff = map_coeffs.customized_copy(
data=map_coeffs.data() / (2j))
if (self.map_coeff.anomalous_flag()):
self.map_coeff = map_coeff.average_bijvoet_mates()
self.file_names = []
if (write_map):
self.file_names = self.write_map_file()
def get_map_values_and_grid_sites_frac(
fmodel,
map_type,
grid_step,
d_min,
apply_sigma_scaling,
apply_volume_scaling,
include_f000,
sel_bb,
use_exact_phases):
#
resolution_factor = grid_step/d_min
mp = mmtbx.masks.mask_master_params.extract()
mp.grid_step_factor = 1./resolution_factor
mmtbx_masks_asu_mask_obj = mmtbx.masks.asu_mask(
xray_structure = fmodel.xray_structure,
d_min = d_min,
mask_params = mp)
bulk_solvent_mask = mmtbx_masks_asu_mask_obj.mask_data_whole_uc()
sel = bulk_solvent_mask > 0
bulk_solvent_mask = bulk_solvent_mask.set_selected(sel, 1)
cr_gr = maptbx.crystal_gridding(
unit_cell = fmodel.xray_structure.unit_cell(),
space_group_info = fmodel.f_obs().space_group_info(),
pre_determined_n_real = bulk_solvent_mask.focus())
from mmtbx import map_tools
from cctbx import miller
#
#mc = map_tools.electron_density_map(fmodel = fmodel).map_coefficients(
# map_type = map_type,
# acentrics_scale = 1.0,
# centrics_pre_scale = 1.0)
if not use_exact_phases:
k = fmodel.k_isotropic()*fmodel.k_anisotropic()
print "flex.mean(k):", flex.mean(k)
f_model = fmodel.f_model()
mc_data = abs(fmodel.f_obs()).data()/k - abs(f_model).data()/k
tmp = miller.array(miller_set = f_model,
data = flex.double(f_model.indices().size(), 1)
).phase_transfer(phase_source = f_model)
mc = miller.array(miller_set = tmp,
data = mc_data * tmp.data())
else:
fmodel.update_all_scales(fast=True, remove_outliers=False)
k = fmodel.k_isotropic()*fmodel.k_anisotropic()
fo = fmodel.f_obs().customized_copy(data = fmodel.f_obs().data()/k)
fo = fo.phase_transfer(phase_source = fmodel.f_model())
fc = fmodel.f_calc().customized_copy(data = fmodel.f_calc().data())
mc = miller.array(miller_set = fo,
data = fo.data()-fc.data())
######## XXX
fft_map = miller.fft_map(
crystal_gridding = cr_gr,
fourier_coefficients = mc)
fft_map.apply_volume_scaling()
map_data = fft_map.real_map_unpadded()
xrs = fmodel.xray_structure
sites_cart = xrs.sites_cart().select(sel_bb)
sel = maptbx.grid_indices_around_sites(
unit_cell = xrs.unit_cell(),
fft_n_real = map_data.focus(),
fft_m_real = map_data.all(),
sites_cart = sites_cart,
site_radii = flex.double(sites_cart.size(), 0.5))
map_in = map_data.select(sel)
mm = flex.mean(map_in)
print "mean in (1):", mm
#
#sites_frac = xrs.sites_frac().select(sel_bb)
#mm = 0
#for sf in sites_frac:
# mm += map_data.eight_point_interpolation(sf)
#mm = mm/sites_frac.size()
#print "mean in (2):", mm
########
#
# Add F000
#reg = fmodel.xray_structure.scattering_type_registry(table = "wk1995")
#f_000 = reg.sum_of_scattering_factors_at_diffraction_angle_0() +\
# 0.4*fmodel.xray_structure.unit_cell().volume()
if(include_f000):
#f_000 = include_f000*fmodel.xray_structure.unit_cell().volume()*0.3
#f_000 = None # XXX
f_000 = abs(mm * xrs.unit_cell().volume())
#f_000 = 0.626*fmodel.xray_structure.unit_cell().volume()*0.35
else:
f_000 = None
print "f_000:", f_000
#print "XXX", include_f000*fmodel.xray_structure.unit_cell().volume()*0.3
#
fft_map = miller.fft_map(
crystal_gridding = cr_gr,
fourier_coefficients = mc,
f_000 = f_000)
#
assert [apply_sigma_scaling, apply_volume_scaling].count(True) == 1
if(apply_sigma_scaling): fft_map.apply_sigma_scaling()
elif(apply_volume_scaling): fft_map.apply_volume_scaling()
else: assert RuntimeError
nx,ny,nz = fft_map.n_real()
map_data = fft_map.real_map_unpadded()
#map_data = map_data * bulk_solvent_mask
print "n_real:", nx,ny,nz, map_data.size()
grid_sites_frac = flex.vec3_double()
map_values = flex.double()
for ix in xrange(nx):
for iy in xrange(ny):
for iz in xrange(nz):
mv = map_data[(ix,iy,iz)]
if 1: #if(mv != 0):
xf,yf,zf = ix/float(nx), iy/float(ny), iz/float(nz)
grid_sites_frac.append([xf,yf,zf])
map_at_ixiyiz = map_data[(ix,iy,iz)]
map_values.append(map_at_ixiyiz)
return map_values, grid_sites_frac
