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https://github.com/cdtools-developers/cdtools.git
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This commit is contained in:
+59
-57
@@ -11,7 +11,7 @@ simulate_to_dataset
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Creates a CDataset from the simulation defined in the model
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save_results
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Saves out a dictionary with the recovered parameters
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Simulation
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----------
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@@ -56,7 +56,7 @@ class CDIModel(t.nn.Module):
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def __init__(self):
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super(CDIModel,self).__init__()
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self.iteration_count = 0
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def from_dataset(self, dataset):
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raise NotImplementedError()
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@@ -79,11 +79,11 @@ class CDIModel(t.nn.Module):
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def forward(self, *args):
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"""The complete forward model
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This model relies on composing the interaction, forward propagator,
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and measurement functions which are required to be defined by all
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subclasses. It therefore should not be redefined by the subclasses.
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The arguments to this function, for any given subclass, will be
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the same as the arguments to the interaction function.
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"""
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@@ -99,7 +99,7 @@ class CDIModel(t.nn.Module):
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def simulate_to_dataset(self, args_list):
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raise NotImplementedError()
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def save_results(self):
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raise NotImplementedError()
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@@ -107,10 +107,10 @@ class CDIModel(t.nn.Module):
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scheduler=None, regularization_factor=None, thread=True,
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calculation_width=10):
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"""Runs a round of reconstruction using the provided optimizer
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This is the basic automatic differentiation reconstruction tool
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which all the other, algorithm-specific tools, use.
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Like all the other optimization routines, it is defined as a
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generator function which yields the average loss each epoch.
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@@ -135,7 +135,7 @@ class CDIModel(t.nn.Module):
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normalization = 0
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for inputs, patterns in data_loader:
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normalization += t.sum(patterns).cpu().numpy()
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def run_iteration(stop_event=None):
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loss = 0
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N = 0
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@@ -144,7 +144,7 @@ class CDIModel(t.nn.Module):
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N += 1
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def closure():
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optimizer.zero_grad()
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input_chunks = [[inp[i:i + calculation_width]
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for inp in inputs]
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for i in range(0, len(inputs[0]),
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@@ -152,7 +152,7 @@ class CDIModel(t.nn.Module):
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pattern_chunks = [patterns[i:i + calculation_width]
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for i in range(0, len(inputs[0]),
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calculation_width)]
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total_loss = 0
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for inp, pats in zip(input_chunks, pattern_chunks):
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# This is just used to allow graceful exit when
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@@ -168,7 +168,7 @@ class CDIModel(t.nn.Module):
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loss = self.loss(pats,sim_patterns)
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loss.backward()
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total_loss += loss.detach()
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if regularization_factor is not None \
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@@ -178,7 +178,7 @@ class CDIModel(t.nn.Module):
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return total_loss
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loss += optimizer.step(closure).detach().cpu().numpy()
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loss /= normalization
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if scheduler is not None:
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scheduler.step(loss)
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@@ -198,7 +198,7 @@ class CDIModel(t.nn.Module):
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# If something bad happens, put the exception into the
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# result queue
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result_queue.put(e)
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for it in range(iterations):
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if thread:
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calc = threading.Thread(target=target, name='calculator', daemon=True)
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@@ -206,10 +206,10 @@ class CDIModel(t.nn.Module):
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calc.start()
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while calc.is_alive():
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if hasattr(self, 'figs'):
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self.figs[0].canvas.start_event_loop(0.01)
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self.figs[0].canvas.start_event_loop(0.01)
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else:
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calc.join()
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except KeyboardInterrupt as e:
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stop_event.set()
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print('\nAsking execution thread to stop cleanly - please be patient.')
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@@ -233,7 +233,7 @@ class CDIModel(t.nn.Module):
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regularization_factor=None, thread=True,
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calculation_width=10):
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"""Runs a round of reconstruction using the Adam optimizer
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This is generally accepted to be the most robust algorithm for use
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with ptychography. Like all the other optimization routines,
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it is defined as a generator function, which yields the average
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@@ -267,7 +267,7 @@ class CDIModel(t.nn.Module):
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if type(subset) == type(1):
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subset = [subset]
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dataset = torchdata.Subset(dataset, subset)
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# Make a dataloader
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data_loader = torchdata.DataLoader(dataset, batch_size=batch_size,
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shuffle=True)
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@@ -290,17 +290,17 @@ class CDIModel(t.nn.Module):
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calculation_width=calculation_width)
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def LBFGS_optimize(self, iterations, dataset,
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def LBFGS_optimize(self, iterations, dataset,
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lr=0.1,history_size=2, subset=None,
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regularization_factor=None, thread=True,
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calculation_width=10):
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"""Runs a round of reconstruction using the L-BFGS optimizer
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This algorithm is often less stable that Adam, however in certain
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situations or geometries it can be shockingly efficient. Like all
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the other optimization routines, it is defined as a generator
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function which yields the average loss each epoch.
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Note: There is no batch size, because it is a usually a bad idea to use
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LBFGS on anything but all the data at onece
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@@ -320,14 +320,14 @@ class CDIModel(t.nn.Module):
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Optional, if the model has a regularizer defined, the set of parameters to pass the regularizer method
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thread : bool
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Default True, whether to run the computation in a separate thread to allow interaction with plots during computation
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"""
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if subset is not None:
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# if just one pattern, turn into a list for convenience
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if type(subset) == type(1):
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subset = [subset]
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dataset = torchdata.Subset(dataset, subset)
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# Make a dataloader. This basically does nothing but load all the
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# data at once
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data_loader = torchdata.DataLoader(dataset, batch_size=len(dataset))
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@@ -338,7 +338,7 @@ class CDIModel(t.nn.Module):
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lr = lr, history_size=history_size)
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#optimizer = MyLBFGS(self.parameters(),
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# lr = lr, history_size=history_size)
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return self.AD_optimize(iterations, data_loader, optimizer,
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regularization_factor=regularization_factor,
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thread=thread,
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@@ -350,7 +350,7 @@ class CDIModel(t.nn.Module):
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nesterov=False, subset=None, regularization_factor=None,
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thread=True, calculation_width=10):
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"""Runs a round of reconstruction using the SGDoptimizer
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This algorithm is often less stable that Adam, but it is simpler
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and is the basic workhorse of gradience descent.
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@@ -382,7 +382,7 @@ class CDIModel(t.nn.Module):
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if type(subset) == type(1):
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subset = [subset]
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dataset = torchdata.Subset(dataset, subset)
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# Make a dataloader
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if batch_size is not None:
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data_loader = torchdata.DataLoader(dataset, batch_size=batch_size,
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@@ -418,28 +418,28 @@ class CDIModel(t.nn.Module):
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self.latest_iteration_time + str(self.latest_loss)
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else:
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return 'No reconstruction iterations performed yet!'
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# By default, the plot_list is empty
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plot_list = []
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def inspect(self, dataset=None, update=True):
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"""Plots all the plots defined in the model's plot_list attribute
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If update is set to True, it will update any previously plotted set
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of plots, if one exists, and then redraw them. Otherwise, it will
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plot a new set, and any subsequent updates will update the new set
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Optionally, a dataset can be passed, which then will plot any
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registered plots which need to incorporate some information from
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the dataset (such as geometry or a comparison with measured data).
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Plots can be registered in any subclass by defining the plot_list
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attribute. This should be a list of tuples in the following format:
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( 'Plot Title', function_to_generate_plot(self),
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( 'Plot Title', function_to_generate_plot(self),
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function_to_determine_whether_to_plot(self))
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Where the third element in the tuple (a function that returns
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Where the third element in the tuple (a function that returns
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True if the plot is relevant) is not required.
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Parameters
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@@ -448,9 +448,9 @@ class CDIModel(t.nn.Module):
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Optional, a dataset matched to the model type
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update : bool
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Default True, whether to update existing plots or plot new ones
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"""
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first_update = False
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if update and hasattr(self, 'figs') and self.figs:
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figs = self.figs
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@@ -476,7 +476,7 @@ class CDIModel(t.nn.Module):
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plotter = plots[1]
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if figs is None:
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fig = plt.figure()
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fig = plt.figure()
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self.figs.append(fig)
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else:
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fig = figs[idx]
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@@ -484,13 +484,13 @@ class CDIModel(t.nn.Module):
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try:
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plotter(self,fig)
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plt.title(name)
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except TypeError as e:
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if dataset is not None:
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try:
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plotter(self, fig, dataset)
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plt.title(name)
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except (IndexError, KeyError, AttributeError, np.linalg.LinAlgError) as e:
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pass
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@@ -498,15 +498,15 @@ class CDIModel(t.nn.Module):
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pass
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idx += 1
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if update:
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plt.draw()
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fig.canvas.start_event_loop(0.001)
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if first_update:
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plt.pause(0.05 * len(self.figs))
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def save_figures(self, prefix='', extension='.eps'):
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"""Saves all currently open inspection figures.
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@@ -520,7 +520,7 @@ class CDIModel(t.nn.Module):
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By default, the files will be named by the figure titles as defined
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in the plot_list. Files can be saved with any extension suported by
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matplotlib.pyplot.savefig.
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Parameters
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----------
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prefix : str
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@@ -528,7 +528,7 @@ class CDIModel(t.nn.Module):
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extention : strategy
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Default is .eps, the file extension to save with.
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"""
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if hasattr(self, 'figs') and self.figs:
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figs = self.figs
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else:
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@@ -538,21 +538,21 @@ class CDIModel(t.nn.Module):
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fig.savefig(prefix + fig.axes[0].get_title() + extension,
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bbox_inches = 'tight')
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def compare(self, dataset):
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def compare(self, dataset, logarithmic=False):
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"""Opens a tool for comparing simulated and measured diffraction patterns
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Parameters
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----------
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dataset : CDataset
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A dataset containing the simulated diffraction patterns to compare against
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"""
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fig, axes = plt.subplots(1,3,figsize=(12,5.3))
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fig.tight_layout(rect=[0.02, 0.09, 0.98, 0.96])
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axslider = plt.axes([0.15,0.06,0.75,0.03])
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def update_colorbar(im):
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# If the update brought the colorbar out of whack
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# (say, from clicking back in the navbar)
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@@ -564,7 +564,7 @@ class CDIModel(t.nn.Module):
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if hasattr(im, 'norecurse') and im.norecurse:
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im.norecurse=False
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return
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im.norecurse=True
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im.set_clim(vmin=np.min(im.get_array()),vmax=np.max(im.get_array()))
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@@ -572,7 +572,7 @@ class CDIModel(t.nn.Module):
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idx = int(idx) % len(dataset)
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fig.pattern_idx = idx
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updating = True if len(axes[0].images) >= 1 else False
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inputs, output = dataset[idx]
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sim_data = self.forward(*inputs).detach().cpu().numpy()
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sim_data = sim_data
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@@ -581,6 +581,10 @@ class CDIModel(t.nn.Module):
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mask = self.mask.detach().cpu().numpy()
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else:
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mask = 1
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if logarithmic:
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sim_data =np.log(sim_data)/np.log(10)
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meas_data = np.log(meas_data)/np.log(10)
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if not updating:
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axes[0].set_title('Simulated')
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@@ -600,7 +604,7 @@ class CDIModel(t.nn.Module):
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cb3 = plt.colorbar(diff, ax=axes[2], orientation='horizontal',format='%.2e',ticks=ticker.LinearLocator(numticks=5),pad=0.1,fraction=0.1)
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cb3.ax.tick_params(labelrotation=20)
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cb3.ax.callbacks.connect('xlim_changed', lambda ax: update_colorbar(diff))
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else:
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sim = axes[0].images[-1]
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@@ -614,8 +618,8 @@ class CDIModel(t.nn.Module):
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diff = axes[2].images[-1]
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diff.set_data((sim_data-meas_data) * mask)
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update_colorbar(diff)
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# This is dumb but the slider doesn't work unless a reference to it is
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# kept somewhere...
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self.slider = Slider(axslider, 'Pattern #', 0, len(dataset)-1, valstep=1, valfmt="%d")
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@@ -626,7 +630,7 @@ class CDIModel(t.nn.Module):
|
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event.button = None
|
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if not hasattr(event, 'key'):
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||||
event.key = None
|
||||
|
||||
|
||||
if event.key == 'up' or event.button == 'up':
|
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update(fig.pattern_idx - 1)
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elif event.key == 'down' or event.button == 'down':
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@@ -637,5 +641,3 @@ class CDIModel(t.nn.Module):
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fig.canvas.mpl_connect('key_press_event',on_action)
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fig.canvas.mpl_connect('scroll_event',on_action)
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update(0)
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||||
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||||
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||||
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@@ -21,13 +21,13 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
detector_slice=None,
|
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surface_normal=np.array([0.,0.,1.]),
|
||||
min_translation = t.Tensor([0,0]),
|
||||
background = None, translation_offsets=None,
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||||
background = None, translation_offsets=None,
|
||||
polarizer_offsets=None, analyzer_offsets=None,
|
||||
polarizer_scale=1, analyzer_scale=1, mask=None,
|
||||
weights = None, translation_scale = 1, saturation=None,
|
||||
probe_support = None, obj_support=None, oversampling=1,
|
||||
loss='amplitude mse',units='um'):
|
||||
|
||||
|
||||
super(FancyPtycho, self).__init__(wavelength, detector_geometry,
|
||||
probe_basis,
|
||||
probe_guess, obj_guess,
|
||||
@@ -48,29 +48,55 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
self.analyzer_offsets = None
|
||||
else:
|
||||
self.analyzer_offsets = t.nn.Parameter(t.tensor(analyzer_offsets).to(dtype=t.float32)) / analyzer_scale
|
||||
|
||||
|
||||
self.polarizer = polarizer
|
||||
self.analyzer = analyzer
|
||||
probe_guess = t.tensor(probe_guess, dtype=t.complex64)
|
||||
if probe_guess.dim() > 4:
|
||||
self.probe_norm = 1 * t.max(t.abs(probe_guess[0]))
|
||||
else:
|
||||
self.probe_norm = 1 * t.max(t.abs(probe_guess))
|
||||
|
||||
self.probe = t.nn.Parameter(probe_guess / self.probe_norm)
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||||
|
||||
@classmethod
|
||||
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', left_polarized=True):
|
||||
|
||||
|
||||
model = FancyPtycho.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, scattering_mode=None, oversampling=1, auto_center=False, opt_for_fft=False, loss='amplitude mse', units='um')
|
||||
|
||||
|
||||
# Mutate the class to its subclass
|
||||
# Mutate the class to its subclass
|
||||
model.__class__ = cls
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||||
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||||
if left_polarized:
|
||||
x = 1j
|
||||
else:
|
||||
x = -1j
|
||||
model.probe.data = t.stack((model.probe.data.to(dtype=t.cfloat), x * model.probe.data.to(dtype=t.cfloat)), dim=-3)
|
||||
obj = t.stack((model.obj.data, model.obj.data), dim=-3)
|
||||
model.obj.data = t.stack((obj, obj), dim=-4)
|
||||
|
||||
# if probe_size is None:
|
||||
# probe = tools.initializers.SHARP_style_probe(dataset, probe_shape, det_slice, propagation_distance=propagation_distance, oversampling=oversampling)
|
||||
# else:
|
||||
# probe = tools.initializers.gaussian_probe(dataset, probe_basis, probe_shape, probe_size, propagation_distance=propagation_distance)
|
||||
probe = model.probe.detach()
|
||||
|
||||
probe = t.stack((probe, probe * x), dim=-3)
|
||||
probe_max = t.max(t.abs(probe))
|
||||
probe_stack = [0.01 * probe_max * t.rand(probe.shape, dtype=probe.dtype) for i in range(n_modes - 1)]
|
||||
probe = t.stack([probe, ] + probe_stack)
|
||||
|
||||
model.probe.data = probe
|
||||
# obj = t.stack((model.obj.data, model.obj.data), dim=-3)
|
||||
# model.obj.data = t.stack((obj.data, obj.data), dim=-4)
|
||||
# obj = t.exp(1j * randomize_ang * (t.rand(obj_size)-0.5))
|
||||
obj = model.obj.detach()
|
||||
obj = t.stack((obj, obj), dim=-3)
|
||||
obj = t.stack((obj, obj), dim=-4)
|
||||
model.obj.data = obj
|
||||
# tensor vs tensor.data
|
||||
return model
|
||||
|
||||
polarizers = [tools.polarization.generate_linear_polarizer(i * 45) for i in range(3)]
|
||||
|
||||
|
||||
# WHAT IS INDEX?
|
||||
def interaction(self, index, translations, polarizer, analyzer, test=False):
|
||||
|
||||
@@ -84,9 +110,9 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
if self.translation_offsets is not None:
|
||||
pix_trans += self.translation_scale * self.translation_offsets[index]
|
||||
|
||||
|
||||
|
||||
# This restricts the basis probes to stay within the probe support
|
||||
basis_prs = self.probe * self.probe_support[...,:,:] # This makes no sense
|
||||
basis_prs = self.probe * self.probe_support[...,:,:] # This makes no sense
|
||||
# self.probe is an Nx2xXxY stach of probes
|
||||
|
||||
# Now we construct the probes for each shot from the basis probes
|
||||
@@ -106,7 +132,7 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
analyzed_exit_waves = polarization.apply_linear_polarizer(exit_waves, analyzer)
|
||||
|
||||
return analyzed_exit_waves
|
||||
|
||||
|
||||
|
||||
def vectorial_wavefields(wavefields, func, *args, **kwargs):
|
||||
wavefields_x = wavefields[..., 0, :, :, :]
|
||||
@@ -122,7 +148,7 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
def backward_propagator(self, wavefields):
|
||||
return tools.propagators.inverse_far_field(wavefields)
|
||||
|
||||
|
||||
|
||||
def measurement(self, wavefields):
|
||||
wavefields_x = wavefields[..., 0, :, :]
|
||||
wavefields_y = wavefields[..., 1, :, :]
|
||||
@@ -145,15 +171,15 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
|
||||
# Note: No "loss" function is defined here, because it is added
|
||||
# dynamically during object creation in __init__
|
||||
|
||||
|
||||
def to(self, *args, **kwargs):
|
||||
super(PolarizedFancyPtycho, self).to(*args, **kwargs)
|
||||
|
||||
|
||||
|
||||
def sim_to_dataset(self, args_list):
|
||||
# In the future, potentially add more control
|
||||
# over what metadata is saved (names, etc.)
|
||||
|
||||
|
||||
# First, I need to gather all the relevant data
|
||||
# that needs to be added to the dataset
|
||||
entry_info = {'program_name': 'CDTools',
|
||||
@@ -166,16 +192,16 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
ysurfacevec = np.cross(surface_normal, xsurfacevec)
|
||||
ysurfacevec /= np.linalg.norm(ysurfacevec)
|
||||
orientation = np.array([xsurfacevec, ysurfacevec, surface_normal])
|
||||
|
||||
|
||||
sample_info = {'description': 'A simulated sample',
|
||||
'orientation': orientation}
|
||||
|
||||
|
||||
|
||||
detector_geometry = self.detector_geometry
|
||||
mask = self.mask
|
||||
wavelength = self.wavelength
|
||||
indices, translations = args_list
|
||||
|
||||
|
||||
# Then we simulate the results
|
||||
data = self.forward(indices, translations)
|
||||
|
||||
@@ -187,14 +213,14 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
detector_geometry=detector_geometry,
|
||||
mask=mask)
|
||||
|
||||
|
||||
|
||||
def corrected_translations(self, dataset):
|
||||
translations = dataset.translations.to(dtype=t.float32,device=self.probe.device)
|
||||
t_offset = tools.interactions.pixel_to_translations(self.probe_basis,self.translation_offsets*self.translation_scale,surface_normal=self.surface_normal)
|
||||
return translations + t_offset
|
||||
|
||||
|
||||
|
||||
|
||||
def get_rhos(self):
|
||||
# If this is the general unified mode model
|
||||
if self.weights.dim() >= 2:
|
||||
@@ -205,18 +231,18 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
else:
|
||||
return np.array([np.eye(self.probe.shape[0])]*self.weights.shape[0],
|
||||
dtype=np.complex64)
|
||||
|
||||
|
||||
def tidy_probes(self, normalization=1, normalize=False):
|
||||
"""Tidies up the probes
|
||||
|
||||
|
||||
What we want to do here is use all the information on all the probes
|
||||
to calculate a natural basis for the experiment, and update all the
|
||||
density matrices to operate in that updated basis
|
||||
|
||||
|
||||
"""
|
||||
|
||||
|
||||
# First we treat the purely incoherent case
|
||||
|
||||
|
||||
# I don't love this pattern of using an if statement with a return
|
||||
# to catch this case, but because it's so much simpler than the
|
||||
# unified mode case I think it's appropriate
|
||||
@@ -228,11 +254,11 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
return
|
||||
|
||||
# This is for the unified mode case
|
||||
|
||||
|
||||
# Note to future: We could probably do this more cleanly with an
|
||||
# SVD directly on the Ws matrix, instead of an eigendecomposition
|
||||
# of the rho matrix.
|
||||
|
||||
|
||||
rhos = self.get_rhos()
|
||||
overall_rho = np.mean(rhos,axis=0)
|
||||
probe = self.probe.detach().cpu().numpy()
|
||||
@@ -248,7 +274,7 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
ortho_probes *= np.sqrt(normalization)
|
||||
|
||||
dm_rank = self.weights.shape[1]
|
||||
|
||||
|
||||
new_Ws = []
|
||||
for rho in new_rhos:
|
||||
# These are returned from smallest to largest - we want to keep
|
||||
@@ -263,14 +289,14 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
# when there are thousands of individual matrices to transform
|
||||
# every time this is called.
|
||||
w = np.maximum(w,0)
|
||||
|
||||
|
||||
new_Ws.append(np.dot(np.diag(np.sqrt(w)),v.transpose()))
|
||||
|
||||
|
||||
new_Ws = np.array(new_Ws)
|
||||
|
||||
self.weights.data = t.as_tensor(new_Ws,
|
||||
dtype=self.weights.dtype,device=self.weights.device)
|
||||
|
||||
|
||||
self.probe.data = t.as_tensor(ortho_probes,
|
||||
device=self.probe.device,dtype=self.probe.dtype)
|
||||
|
||||
@@ -287,32 +313,32 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
return np.sum(np.abs(ortho_probes.detach().cpu().numpy())**2,axis=0)
|
||||
if mode.lower() == 'phase':
|
||||
return np.angle(ortho_probes.detach().cpu().numpy())
|
||||
|
||||
|
||||
probe_matrix = np.zeros([self.probe.shape[0]]*2,
|
||||
dtype=np.complex64)
|
||||
np_probes = self.probe.detach().cpu().numpy()
|
||||
for i in range(probe_matrix.shape[0]):
|
||||
for j in range(probe_matrix.shape[0]):
|
||||
probe_matrix[i,j] = np.sum(np_probes[i]*np_probes[j].conj())
|
||||
|
||||
|
||||
|
||||
weights = self.weights.detach().cpu().numpy()
|
||||
|
||||
|
||||
probe_intensities = np.sum(np.tensordot(weights,probe_matrix,axes=1)*
|
||||
weights.conj(),axis=2)
|
||||
|
||||
# Imaginary part is already essentially zero up to rounding error
|
||||
probe_intensities = np.real(probe_intensities)
|
||||
|
||||
|
||||
values = np.sum(probe_intensities,axis=1)
|
||||
if mode.lower() == 'amplitude' or mode.lower() == 'root_sum_intensity':
|
||||
cmap = 'viridis'
|
||||
else:
|
||||
cmap = 'twilight'
|
||||
|
||||
|
||||
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),
|
||||
|
||||
|
||||
|
||||
plot_list = [
|
||||
('',
|
||||
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'),
|
||||
@@ -333,7 +359,7 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
('% Power in Top Mode (only accurate after tidy_probes)',
|
||||
lambda self, fig, dataset: p.plot_nanomap(self.corrected_translations(dataset), analysis.calc_top_mode_fraction(self.get_rhos()), fig=fig,units=self.units),
|
||||
lambda self: len(self.weights.shape) >=2),
|
||||
('Object Amplitude',
|
||||
('Object Amplitude',
|
||||
lambda self, fig: p.plot_amplitude(self.obj, fig=fig, basis=self.probe_basis,units=self.units)),
|
||||
('Object Phase',
|
||||
lambda self, fig: p.plot_phase(self.obj, fig=fig, basis=self.probe_basis,units=self.units)),
|
||||
@@ -343,7 +369,7 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
lambda self, fig: plt.figure(fig.number) and plt.imshow(self.background.detach().cpu().numpy()**2))
|
||||
]
|
||||
|
||||
|
||||
|
||||
def save_results(self, dataset):
|
||||
basis = self.probe_basis.detach().cpu().numpy()
|
||||
translations = self.corrected_translations(dataset).detach().cpu().numpy()
|
||||
@@ -352,7 +378,7 @@ class PolarizedFancyPtycho(FancyPtycho):
|
||||
obj = self.obj.detach().cpu().numpy()
|
||||
background = self.background.detach().cpu().numpy()**2
|
||||
weights = self.weights.detach().cpu().numpy()
|
||||
|
||||
|
||||
return {'basis':basis, 'translation':translations,
|
||||
'probe':probe,'obj':obj,
|
||||
'background':background,
|
||||
|
||||
+107
-62
@@ -1,7 +1,8 @@
|
||||
import numpy as np
|
||||
import torch as t
|
||||
from scipy import misc
|
||||
from CDTools.models import PolarizedFancyPtycho
|
||||
#from CDTools.datasets import Polarized2DDataset
|
||||
from CDTools.datasets import PolarizedPtycho2DDataset
|
||||
import CDTools
|
||||
from CDTools.tools import polarization
|
||||
from CDTools import tools
|
||||
@@ -11,77 +12,121 @@ from PIL import Image
|
||||
# upolad 4 different images representing 4 components of the object
|
||||
# and 2 gaaussian functionas corresponding to the probe components
|
||||
|
||||
a = np.asarray(Image.open('a.jpg'))
|
||||
b = np.asarray(Image.open('b.jpg'))
|
||||
c = np.asarray(Image.open('c.jpg'))
|
||||
d = np.asarray(Image.open('d.jpg'))
|
||||
f = misc.ascent()
|
||||
x , y = np.shape(f)
|
||||
aa = f[:x//2, :y//2]
|
||||
bb = f[:x//2, -y//2:]
|
||||
cc = f[-x//2:, :y//2]
|
||||
dd = f[-x//2:, -y//2:]
|
||||
|
||||
#a = np.dot(a[..., :3], [.3, 6., .1])
|
||||
print(1)
|
||||
|
||||
def simulate_dataset(probe_size, obj_size, num_patt):
|
||||
translations = []
|
||||
xs, ys = np.mgrid[:num_patt, :num_patt]
|
||||
for x, y in zip(xs, ys):
|
||||
translations.append((x*10e-3, y*10e-3))
|
||||
|
||||
translations = t.as_tensor(translations, dtype=t.float32)
|
||||
a = t.as_tensor(a, dtype=t.cfloat)
|
||||
a = t.tensordot(a, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1],[0]))[:obj_size, :obj_size]
|
||||
|
||||
probe = tools.initializers.gaussian(np.array([probe_size, probe_size]), 50)
|
||||
wavefields = tools.interactions.ptycho_2D_sinc(probe, obj, translations)
|
||||
patterns = tools.propagators.far_field(wavefront)
|
||||
patterns = np(patterns)
|
||||
translations = np(t.cat((translations, t.zeros(num_patt)), dim=-1))
|
||||
|
||||
# needs to be stored as a cxi file
|
||||
dataset = CDTools.datasets.Ptycho2DDataset.from_cxi('simulated_dataset.cxi')
|
||||
dataset.detector_geometry = None
|
||||
|
||||
def simulate polarized_datset(probe_size, obj_size, num_patt):
|
||||
def simulate_polarized_dataset(probe_size, obj_size, num_patt, a, b, c, d):
|
||||
a, b, c, d = t.as_tensor(a, dtype=t.cfloat), t.as_tensor(b, dtype=t.cfloat), t.as_tensor(c, dtype=t.cfloat), t.as_tensor(d, dtype=t.cfloat)
|
||||
a = t.tensordot(a, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1],[0]))[:obj_size, :obj_size]
|
||||
b = t.tensordot(b, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1], [0]))[:obj_size, :obj_size]
|
||||
c = t.tensordot(c, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1], [0]))[:obj_size, :obj_size]
|
||||
d = t.tensordot(d, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1], [0]))[:obj_size, :obj_size]
|
||||
|
||||
# a = t.tensordot(a, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1],[0]))[:obj_size, :obj_size]
|
||||
# b = t.tensordot(b, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1], [0]))[:obj_size, :obj_size]
|
||||
# c = t.tensordot(c, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1], [0]))[:obj_size, :obj_size]
|
||||
# d = t.tensordot(d, t.tensor([.3, .6, .1], dtype=t.cfloat), dims=([-1], [0]))[:obj_size, :obj_size]
|
||||
|
||||
translations = []
|
||||
xs, ys = np.mgrid[:num_patt, :num_patt]
|
||||
xs, ys = np.ravel(xs), np.ravel(ys)
|
||||
for x, y in zip(xs, ys):
|
||||
translations.append((x*10e-3, y*10e-3))
|
||||
for j in range(9):
|
||||
translations.append((5*x, 5*y))
|
||||
translations = t.as_tensor(translations, dtype=t.float32)
|
||||
|
||||
obj = t.stack((t.stack((a, c), dim=0), t.stack((b, d), dim=0)), dim=-3)
|
||||
probe = tools.initializers.gaussian(np.array([probe_size, probe_size]), 50)
|
||||
obj = t.stack((t.stack((a, b), dim=-3), t.stack((c, d), dim=-3)), dim=-4)
|
||||
|
||||
# for i, j in zip([0, 0, 1, 1], [0, 1, 0, 1]):
|
||||
# plt.imshow(np.real(obj[i, j, ...]))
|
||||
# plt.show()
|
||||
probe = tools.initializers.gaussian(np.array([probe_size, probe_size]), np.array((2, 2)))
|
||||
probe = t.stack((probe, probe), dim=-3)
|
||||
probe = polarization.apply_circular_polarizer(probe)
|
||||
probe = polarization.apply_circular_polarizer(probe, multiple_modes=False)
|
||||
polarizers = polarization.generate_linear_polarizer(t.tensor([0, 45, 90]))
|
||||
num_transl = len(translations)
|
||||
pol_probes = [polarization.apply_jones_matrix(probe, polarizers[i], multiple_modes=False) for i in range(3)]
|
||||
analyzers = t.stack(([polarizers[i % 3] for i in range(num_transl)]), dim=0)
|
||||
analyzer = t.tensor([(i % 3) * 45 for i in range(num_transl)])
|
||||
polarizer = t.tensor([(i // 3) % 3 * 45 for i in range(num_transl)])
|
||||
polarized_probes = t.stack(([pol_probes[(i // 3) % 3] for i in range(num_transl)]), dim=0)
|
||||
polarized_wavefields = t.stack([tools.interactions.ptycho_2D_sinc(polarized_probes[i], obj, translations[i], polarized=True, multiple_modes=False) for i in range(num_transl)])
|
||||
wavefields = tools.propagators.far_field(polarized_wavefields)
|
||||
wavefields = polarization.apply_jones_matrix(wavefields, analyzers, multiple_modes=False)
|
||||
patterns = t.abs(wavefields[:, 0, :, :])**2 + t.abs(wavefields[:, 1, :, :])**2
|
||||
detector_basis = t.transpose(t.tensor([[0, -4.8e-6, 0], [-4.8e-6, 0, 0]]), 0, 1)
|
||||
det_shape = t.Size((obj_size, obj_size))
|
||||
wavelength = 532e-9
|
||||
real_basis = tools.initializers.exit_wave_geometry(detector_basis, det_shape, wavelength, 2.5e-2)[0]
|
||||
# print('f', type(real_basis), translations.shape)
|
||||
real_translations = tools.interactions.pixel_to_translations(real_basis, translations)
|
||||
# print(type(real_translations))
|
||||
patterns = patterns.numpy()
|
||||
detector_geometry = {
|
||||
'corner': np.array([probe_size*4.8e-6/2, probe_size*4.8e-6/2, 2.5e-2]),
|
||||
'basis': np.array([[0, -4.8e-6, 0], [-4.8e-6, 0, 0]]).transpose(),
|
||||
'distance': 2.5e-2
|
||||
}
|
||||
|
||||
selections = tools.interactions.ptycho_2D_sinc(t.ones(2, probe_size, probe_size).to(dtype=t.cfloat), obj, translations, polarized=True)
|
||||
polarizers = [polarization.generate_linear_polarizer(i * 45) for i in range(3)]
|
||||
|
||||
pol_probes = [polarization.apply_jones_matrix(probe, polarizers[i]) for i in range(3)]
|
||||
|
||||
return PolarizedPtycho2DDataset(real_translations, polarizer, analyzer, patterns,
|
||||
axes=("x", "y"), detector_geometry=detector_geometry, wavelength=wavelength)
|
||||
|
||||
analyzer = t.stack(([polaryzers[i % 3] for i in range(num_patt)]), dim=0)
|
||||
# probes = t.stack(([probes[i // 3] for i in num_patt]), dim=0)
|
||||
wavefields = t.as_tensor([tools.interactions.ptycho_2D_sinc(pol_probes[i], obj, translations, polarized=True) for i in range(3)]).to(dtype=t.cfloat)
|
||||
# print(1)
|
||||
dataset = simulate_polarized_dataset(100, 500, 10, aa, bb, cc, dd)
|
||||
# print(2)
|
||||
dataset.inspect()
|
||||
# print(3)
|
||||
plt.show()
|
||||
model = PolarizedFancyPtycho.from_dataset(dataset, propagation_distance=1e-3)
|
||||
model.inspect()
|
||||
# plt.show()
|
||||
model.compare(dataset)
|
||||
plt.show()
|
||||
|
||||
wf = t.empty(1, 2, obj_size, obj_size)
|
||||
for i in range(num_patt):
|
||||
for j in range(3):
|
||||
pol_channel = t.stack(([wavefileds[j] for k in range(3)]), dim=0)
|
||||
wf = t.cat((wf, pol_channel), dim=0)
|
||||
|
||||
pol_wavefieds = polarization.apply_jones_matrix(wf, analyzer)
|
||||
# for loss in model.Adam_optimize(400, dataset, batch_size=5, lr=0.002, schedule=True):
|
||||
# # And we liveplot the updates to the model as they happen
|
||||
# print(model.report())
|
||||
# model.inspect(dataset)
|
||||
# model.save_figures(prefix='simulated', extension='png')
|
||||
# res = model.save_results(dataset)
|
||||
# np.save('simulated_dataset.npy', res)
|
||||
|
||||
patterns = tools.propagators.far_field(pol_wavefieds)
|
||||
dataset = simulate_polarized_dataset(50, 100, 10, aa, bb, cc, dd)
|
||||
|
||||
translations = np(t.cat((translations, t.zeros(num_patt)), dim=-1))
|
||||
patterns = np(patterns)
|
||||
dataset.detector_geometry = None
|
||||
# needs to be stored in a cxi file
|
||||
dataset = CDTools.datasets.FancyPtycho2DDataset.from_cxi('polarized_simulated_dataset.cxi')
|
||||
dataset.inspect()
|
||||
|
||||
|
||||
model = tools.models.PolarizedFancyPtycho.from_dataset(dataset)
|
||||
res = np.load('simulated_dataset.npy', allow_pickle=True)
|
||||
res = res[()]
|
||||
print(type(res))
|
||||
Ws = t.ones(len(dataset))
|
||||
ewg = CDTools.tools.initializers.exit_wave_geometry
|
||||
probe_basis, probe_shape, det_slice = ewg(res['basis'],
|
||||
dataset[0][1].shape,
|
||||
dataset.wavelength,
|
||||
dataset.detector_geometry['distance'],
|
||||
center=None,
|
||||
padding=0)
|
||||
print('object', res['obj'].shape)
|
||||
obj = res['obj'][..., 200:275, 200:275]
|
||||
# print('obj', obj)
|
||||
a = obj[0, 0, :, :]
|
||||
b = obj[0, 1, :, :]
|
||||
c = obj[1, 0, :, :]
|
||||
d = obj[1, 1, :, :]
|
||||
for i in [a, b, c, d]:
|
||||
plt.imshow(np.real(i))
|
||||
# plt.imshow(np.log(np))
|
||||
plt.colorbar()
|
||||
plt.show()
|
||||
print(np.allclose(np.real(a), np.real(b)))
|
||||
print('a', a[..., 10:20, 10:20])
|
||||
print('b', b[..., 10:20, 10:20])
|
||||
models = [CDTools.models.FancyPtycho(dataset.wavelength, dataset.detector_geometry, probe_basis,
|
||||
res['probe'], component, surface_normal=t.tensor([0., 0., 1.], dtype=t.float32),
|
||||
min_translation=t.tensor([0, 0], dtype=t.float32),
|
||||
background=t.tensor(res['background']), translation_offsets=None, mask=None,
|
||||
weights=Ws, translation_scale=1, saturation=None,
|
||||
probe_support=None, oversampling=1,
|
||||
loss='amplitude mse', units='um') for component in [a, b, c, d]]
|
||||
# print('model is created')
|
||||
# for model in models:
|
||||
# model.inspect()
|
||||
# plt.show()
|
||||
|
||||
Reference in New Issue
Block a user