mirror of
https://github.com/cdtools-developers/cdtools.git
synced 2026-09-09 21:12:42 +02:00
not tested/debugged yet
This commit is contained in:
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cd ..
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_future__ import division, print_function, absolute_import
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import torch as t
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from CDTools.models import CDIModel, FancyPtycho
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from CDTools.datasets import Ptycho2DDataset
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from CDTools import tools
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from CDTools.tools import plotting as p
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from CDTools.tools import analysis
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from matplotlib import pyplot as plt
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from datetime import datetime
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import numpy as np
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from scipy import linalg as sla
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from copy import copy
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__all__ = ['PolarizedFancyPtycho']
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class PolarizedFancyPtycho(FancyPtycho):
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def __init__(self, wavelength, detector_geometry,
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probe_basis,
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probe_guess, obj_guess,
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detector_slice=None,
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surface_normal=np.array([0.,0.,1.]),
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min_translation = t.Tensor([0,0]),
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background = None, translation_offsets=None,
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polarizer_offsets=None, analyzer_offsets=None,
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polarizer_scale=1, analyzer_scale=1, mask=None,
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weights = None, translation_scale = 1, saturation=None,
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probe_support = None, obj_support=None, oversampling=1,
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loss='amplitude mse',units='um', polarizer, analyzer):
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super(FancyPtycho, self).__init__(wavelength, detector_geometry,
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probe_basis,
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probe_guess, obj_guess,
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detector_slice=None,
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surface_normal=np.array([0.,0.,1.]),
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min_translation = t.Tensor([0,0]),
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background = None, translation_offsets=None, mask=None,
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weights = None, translation_scale = 1, saturation=None,
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probe_support = None, obj_support=None, oversampling=1,
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loss='amplitude mse',units='um')
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if polarizer_offsets is None:
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self.polarizer_offsets = None
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else:
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self.polarizer_offsets = t.nn.Parameter(t.tensor(polarizer_offsets).to(dtype=t.float32)) / polarizer_scale
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if analyzer_offsets is None:
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self.analyzer_offsets = None
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else:
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self.analyzer_offsets = t.nn.Parameter(t.tensor(analyzer_offsets).to(dtype=t.float32)) / analyzer_scale
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@classmethod
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def from_dataset(cls, dataset, probe_size=None, randomize_ang=0, padding=0, n_modes=1, dm_rank=None, translation_scale = 1, saturation=None, probe_support_radius=None, propagation_distance=None, restrict_obj=-1, scattering_mode=None, oversampling=1, auto_center=False, opt_for_fft=False, loss='amplitude mse', units='um'):
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super(PolarizedFancyPtycho, cls).from_dataset(dataset, probe_size=None, randomize_ang=0, padding=0, n_modes=1, dm_rank=None, translation_scale = 1, saturation=None, probe_support_radius=None, propagation_distance=None, restrict_obj=-1, scattering_mode=None, oversampling=1, auto_center=False, opt_for_fft=False, loss='amplitude mse', units='um')
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# always do this on the cpu
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get_as_args = dataset.get_as_args
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dataset.get_as(device='cpu')
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(indices, translations), patterns = dataset[:]
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dataset.get_as(*get_as_args[0],**get_as_args[1])
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# Set to none to avoid issues with things outside the detector
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ewg = tools.initializers.exit_wave_geometry
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probe_basis, probe_shape, det_slice = ewg(det_basis,
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det_shape,
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wavelength,
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distance,
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center=center,
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padding=padding,
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opt_for_fft=opt_for_fft,
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oversampling=oversampling)
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scalar_probe_shape = probe_shape.clone()
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probe_shape = t.stack((probe_shape[:-2], t.tensor([2, 1]), probe_shape([-2:])))
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obj_size, min_translation = tools.initializers.calc_object_setup(scalar_probe_shape, pix_translations, padding=200)
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obj_size = t.cat((t.tensor([2, 2]), obj_size))
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# Finally, initialize the probe and object using this information
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if probe_size is None:
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probe = tools.initializers.SHARP_style_probe(dataset, scalar_probe_shape, det_slice, propagation_distance=propagation_distance, oversampling=oversampling, polarized=True)
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else:
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probe = tools.initializers.gaussian_probe(dataset, probe_basis, scalar_probe_shape, probe_size, propagation_distance=propagation_distance, polarized=True)
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return cls(wavelength, det_geo, probe_basis, probe, obj,
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detector_slice=det_slice,
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surface_normal=surface_normal,
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min_translation=min_translation,
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translation_offsets = translation_offsets,
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weights=Ws, mask=mask, background=background,
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translation_scale=translation_scale,
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saturation=saturation,
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probe_support=probe_support,
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obj_support=obj_support,
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oversampling=oversampling,
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loss=loss,units=units)
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def interaction(self, index, translations, polarizer, analyzer):
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# Step 1 is to convert the translations for each position into a
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# value in pixels
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pix_trans = tools.interactions.translations_to_pixel(self.probe_basis,
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translations,
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surface_normal=self.surface_normal)
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pix_trans -= self.min_translation
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# We then add on any recovered translation offset, if they exist
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if self.translation_offsets is not None:
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pix_trans += self.translation_scale * self.translation_offsets[index]
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# This restricts the basis probes to stay within the probe support
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basis_prs = self.probe * self.probe_support[...,:,:]
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# Now we construct the probes for each shot from the basis probes
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Ws = self.weights[index]
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if len(self.weights[0].shape) == 0:
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# If a purely stable coherent illumination is defined
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prs = Ws[...,None,None,None] * basis_prs
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else:
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# If a frame-by-frame weight matrix is defined
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# This takes the dot product of all the weight matrices with
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# the probes. The output has dimensions of translation, then
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# coherent mode index, then x,y, and then complex index
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# Maybe this can be done with a matmul now?
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prs = t.sum(Ws[...,None,None] * basis_prs, axis=-3)
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# Now we actually do the interaction, using the sinc subpixel
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# translation model as per usual
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# I DON'T KNOW WHAT PROBE NORM IS (AS WELL AS OBJ SUPP AND PROBE SUPP)
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exit_waves = self.probe_norm * tools.interactions.ptycho_2D_sinc(
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prs, self.obj_support * self.obj,pix_trans,
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shift_probe=True, multiple_modes=True, polarized=True, polarizer=polarizer, analyzer=analyzer)
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#exit_waves = self.probe_norm * tools.interactions.ptycho_2D_round(
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# prs, self.obj_support * self.obj,pix_trans,
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# multiple_modes=True)
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return exit_waves
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def vectorial_wavefields(wavefields, func, *args. **kwargs):
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wavefields_x = wavefields[..., 0, :, :, :]
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wavefields_y = wavefields[..., 1, :, :, :]
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out_x = func(wavefields_x. *args, **kwargs)
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out_y = func(wavefields_y, *args, **kwargs)
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out = t.stack((out_x, out_y), dim=-4)
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return out[..., None, :, :]
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def forward_propagator(self, wavefields):
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return vectorial_wavefields(wavefields, tools.propagators.far_field)
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def backward_propagator(self, wavefields):
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return vectorial_wavefields(wavefields, tools.propagators.inverse_far_field)
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def measurement(self, wavefields):
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wavefields_x = wavefields[..., 0, :, :, :]
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wavefields_x = wavefields[..., 1, :, :, :]
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out_x = tools.measurements.quadratic_background(wavefields_x,
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self.background,
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detector_slice=self.detector_slice,
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measurement=tools.measurements.incoherent_sum,
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saturation=self.saturation,
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oversampling=self.oversampling)
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# now, set bckgr to 0 since t shouldn't be calculated twice
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out_y = tools.measurements.quadratic_background(wavefields_y,
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0,
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detector_slice=self.detector_slice,
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measurement=tools.measurements.incoherent_sum,
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saturation=self.saturation,
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oversampling=self.oversampling)
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return out_x + out_y
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# Note: No "loss" function is defined here, because it is added
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# dynamically during object creation in __init__
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def to(self, *args, **kwargs):
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super(PolarizedFancyPtycho, self).to(*args, **kwargs)
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def sim_to_dataset(self, args_list):
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# In the future, potentially add more control
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# over what metadata is saved (names, etc.)
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# First, I need to gather all the relevant data
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# that needs to be added to the dataset
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entry_info = {'program_name': 'CDTools',
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'instrument_n': 'Simulated Data',
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'start_time': datetime.now()}
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surface_normal = self.surface_normal.detach().cpu().numpy()
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xsurfacevec = np.cross(np.array([0.,1.,0.]), surface_normal)
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xsurfacevec /= np.linalg.norm(xsurfacevec)
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ysurfacevec = np.cross(surface_normal, xsurfacevec)
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ysurfacevec /= np.linalg.norm(ysurfacevec)
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orientation = np.array([xsurfacevec, ysurfacevec, surface_normal])
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sample_info = {'description': 'A simulated sample',
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'orientation': orientation}
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detector_geometry = self.detector_geometry
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mask = self.mask
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wavelength = self.wavelength
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indices, translations = args_list
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# Then we simulate the results
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data = self.forward(indices, translations)
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# And finally, we make the dataset
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return Ptycho2DDataset(translations, data,
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entry_info = entry_info,
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sample_info = sample_info,
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wavelength=wavelength,
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detector_geometry=detector_geometry,
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mask=mask)
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def corrected_translations(self, dataset):
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translations = dataset.translations.to(dtype=t.float32,device=self.probe.device)
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t_offset = tools.interactions.pixel_to_translations(self.probe_basis,self.translation_offsets*self.translation_scale,surface_normal=self.surface_normal)
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return translations + t_offset
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def get_rhos(self):
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# If this is the general unified mode model
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if self.weights.dim() >= 2:
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Ws = self.weights.detach().cpu().numpy()
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rhos_out = np.matmul(np.swapaxes(Ws,1,2), Ws.conj())
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return rhos_out
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# This is the purely incoherent case
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else:
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return np.array([np.eye(self.probe.shape[0])]*self.weights.shape[0],
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dtype=np.complex64)
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def tidy_probes(self, normalization=1, normalize=False):
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"""Tidies up the probes
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What we want to do here is use all the information on all the probes
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to calculate a natural basis for the experiment, and update all the
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density matrices to operate in that updated basis
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"""
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# First we treat the purely incoherent case
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# I don't love this pattern of using an if statement with a return
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# to catch this case, but because it's so much simpler than the
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# unified mode case I think it's appropriate
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if self.weights.dim() == 1:
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probe = self.probe.detach().cpu().numpy()
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ortho_probes = analysis.orthogonalize_probes(probe)
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self.probe.data = t.as_tensor(ortho_probes,
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device=self.probe.device,dtype=self.probe.dtype)
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return
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# This is for the unified mode case
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# Note to future: We could probably do this more cleanly with an
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# SVD directly on the Ws matrix, instead of an eigendecomposition
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# of the rho matrix.
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rhos = self.get_rhos()
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overall_rho = np.mean(rhos,axis=0)
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probe = self.probe.detach().cpu().numpy()
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ortho_probes, A = analysis.orthogonalize_probes(probe,
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density_matrix=overall_rho,
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keep_transform=True,
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normalize=normalize)
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Aconj = A.conj()
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Atrans = np.transpose(A)
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new_rhos = np.matmul(Atrans,np.matmul(rhos,Aconj))
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new_rhos /= normalization
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ortho_probes *= np.sqrt(normalization)
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dm_rank = self.weights.shape[1]
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new_Ws = []
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for rho in new_rhos:
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# These are returned from smallest to largest - we want to keep
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# the largest ones
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w,v = sla.eigh(rho)
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w = w[::-1][:dm_rank]
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v = v[:,::-1][:,:dm_rank]
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# For situations where the rank of the density matrix is not
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# full in reality, but we keep more modes around than needed,
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# some ws can go negative due to numerical error! This is
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# extremely rare, but comon enough to cause crashes occasionally
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# when there are thousands of individual matrices to transform
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# every time this is called.
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w = np.maximum(w,0)
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new_Ws.append(np.dot(np.diag(np.sqrt(w)),v.transpose()))
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new_Ws = np.array(new_Ws)
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self.weights.data = t.as_tensor(new_Ws,
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dtype=self.weights.dtype,device=self.weights.device)
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self.probe.data = t.as_tensor(ortho_probes,
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device=self.probe.device,dtype=self.probe.dtype)
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def plot_wavefront_variation(self, dataset,fig=None,mode='amplitude',**kwargs):
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def get_probes(idx):
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basis_prs = self.probe * self.probe_support[...,:,:]
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prs = t.sum(self.weights[idx,:,:,None,None] * basis_prs, axis=-4)
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ortho_probes = analysis.orthogonalize_probes(prs)
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if mode.lower() == 'amplitude':
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return np.abs(ortho_probes.detach().cpu().numpy())
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if mode.lower() == 'root_sum_intensity':
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return np.sum(np.abs(ortho_probes.detach().cpu().numpy())**2,axis=0)
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if mode.lower() == 'phase':
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return np.angle(ortho_probes.detach().cpu().numpy())
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probe_matrix = np.zeros([self.probe.shape[0]]*2,
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dtype=np.complex64)
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np_probes = self.probe.detach().cpu().numpy()
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for i in range(probe_matrix.shape[0]):
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for j in range(probe_matrix.shape[0]):
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probe_matrix[i,j] = np.sum(np_probes[i]*np_probes[j].conj())
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weights = self.weights.detach().cpu().numpy()
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probe_intensities = np.sum(np.tensordot(weights,probe_matrix,axes=1)*
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weights.conj(),axis=2)
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# Imaginary part is already essentially zero up to rounding error
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probe_intensities = np.real(probe_intensities)
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values = np.sum(probe_intensities,axis=1)
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if mode.lower() == 'amplitude' or mode.lower() == 'root_sum_intensity':
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cmap = 'viridis'
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else:
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cmap = 'twilight'
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p.plot_nanomap_with_images(self.corrected_translations(dataset), get_probes, values=values, fig=fig, units=self.units, basis=self.probe_basis, nanomap_colorbar_title='Total Probe Intensity',cmap=cmap,**kwargs),
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plot_list = [
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('',
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lambda self, fig, dataset: self.plot_wavefront_variation(dataset,fig=fig,mode='root_sum_intensity',image_title='Root Summed Probe Intensities',image_colorbar_title='Square Root of Intensity'),
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lambda self: len(self.weights.shape) >= 2),
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('',
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lambda self, fig, dataset: self.plot_wavefront_variation(dataset,fig=fig,mode='amplitude',image_title='Probe Amplitudes (scroll to view modes)',image_colorbar_title='Probe Amplitude'),
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lambda self: len(self.weights.shape) >= 2),
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('',
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lambda self, fig, dataset: self.plot_wavefront_variation(dataset,fig=fig,mode='phase',image_title='Probe Phases (scroll to view modes)',image_colorbar_title='Probe Phase'),
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lambda self: len(self.weights.shape) >= 2),
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('Basis Probe Amplitudes (scroll to view modes)',
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lambda self, fig: p.plot_amplitude(self.probe, fig=fig, basis=self.probe_basis,units=self.units)),
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('Basis Probe Phases (scroll to view modes)',
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lambda self, fig: p.plot_phase(self.probe, fig=fig, basis=self.probe_basis,units=self.units)),
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('Average Density Matrix Amplitudes',
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lambda self, fig: p.plot_amplitude(np.nanmean(np.abs(self.get_rhos()),axis=0), fig=fig),
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lambda self: len(self.weights.shape) >=2),
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('% Power in Top Mode (only accurate after tidy_probes)',
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lambda self, fig, dataset: p.plot_nanomap(self.corrected_translations(dataset), analysis.calc_top_mode_fraction(self.get_rhos()), fig=fig,units=self.units),
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lambda self: len(self.weights.shape) >=2),
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('Object Amplitude',
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lambda self, fig: p.plot_amplitude(self.obj, fig=fig, basis=self.probe_basis,units=self.units)),
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('Object Phase',
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lambda self, fig: p.plot_phase(self.obj, fig=fig, basis=self.probe_basis,units=self.units)),
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('Corrected Translations',
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lambda self, fig, dataset: p.plot_translations(self.corrected_translations(dataset), fig=fig,units=self.units)),
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('Background',
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lambda self, fig: plt.figure(fig.number) and plt.imshow(self.background.detach().cpu().numpy()**2))
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]
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def save_results(self, dataset):
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basis = self.probe_basis.detach().cpu().numpy()
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translations = self.corrected_translations(dataset).detach().cpu().numpy()
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probe = self.probe.detach().cpu().numpy()
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probe = probe * self.probe_norm.detach().cpu().numpy()
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obj = self.obj.detach().cpu().numpy()
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background = self.background.detach().cpu().numpy()**2
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weights = self.weights.detach().cpu().numpy()
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return {'basis':basis, 'translation':translations,
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'probe':probe,'obj':obj,
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'background':background,
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'weights':weights}
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