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645 lines
22 KiB
Python
645 lines
22 KiB
Python
#this code implements metapeg_v2 but without imposing the binarization
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#of the design variables. This is useful to test the objective function alone
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import faulthandler
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faulthandler.enable()
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from typing import List, NamedTuple, Tuple
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from autograd import numpy as npa, tensor_jacobian_product, grad
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import matplotlib.pyplot as plt
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import matplotlib.animation as animation
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import meep as mp
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import meep.adjoint as mpa
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import nlopt
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import numpy as np
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import os
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import xarray as xr
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from PIL import Image
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import pickle
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mp.verbosity(3)
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if mp.am_master():
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if not os.path.exists("results"):
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os.makedirs("results")
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###### PHYSICS SETUP ######
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RESOLUTION = 5 #pixels per meep unit length (1um)
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MAX_RUN_TIME = 70 #meep units
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WAVELENGTH_MIN_UM = 1.50
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WAVELENGTH_MAX_UM = 1.60
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PML_UM = 1.0 #PML thickness
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BUFFER = 3.0
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DESIGN_WAVELENGTHS_UM = (1.50,1.55,1.60) #wavelengths at which to optimize the device
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DESIGN_REGION_UM = mp.Vector3(4,4,1)
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DESIGN_REGION_RESOLUTION = int(RESOLUTION)
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DESIGN_REGION_CENTER = mp.Vector3(0, 0, DESIGN_REGION_UM.z / 2)
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NX_DESIGN_GRID = int(DESIGN_REGION_UM.x * DESIGN_REGION_RESOLUTION) + 1
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NY_DESIGN_GRID = int(DESIGN_REGION_UM.y * DESIGN_REGION_RESOLUTION) + 1
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MIN_LENGTH_UM = 0.5 #500 nm minimum length scale
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SILICON = mp.Medium(index = 3.5)
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SILICON_DIOXIDE = mp.Medium(index = 1.5)
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AIR = mp.Medium(index = 1.0)
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cell_um = mp.Vector3(
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DESIGN_REGION_UM.x + 2*BUFFER + 2*PML_UM,
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DESIGN_REGION_UM.y + 2*BUFFER + 2*PML_UM,
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2*BUFFER + 2*PML_UM
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)
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SUBSTRATE_THICKNESS = BUFFER + PML_UM
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SUBSTRATE_SIZE = mp.Vector3(cell_um.x, cell_um.y, SUBSTRATE_THICKNESS)
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SUBSTRATE_CENTER = mp.Vector3(0, 0, -SUBSTRATE_THICKNESS/2)
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physical_domains_size = mp.Vector3(
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DESIGN_REGION_UM.x + 2*BUFFER,
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DESIGN_REGION_UM.y + 2*BUFFER,
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2*BUFFER
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)
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frequency_min = 1 / WAVELENGTH_MAX_UM
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frequency_max = 1 / WAVELENGTH_MIN_UM
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frequency_center = 0.5 * (frequency_min + frequency_max)
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wavelength_center = 1 / frequency_center #remember that c = 1 in meep units
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frequency_width = frequency_max - frequency_min
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frequencies = [1/wavelength for wavelength in DESIGN_WAVELENGTHS_UM]
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num_wavelengths = len(DESIGN_WAVELENGTHS_UM)
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SOURCE_CENTER = mp.Vector3(0,0,-BUFFER/2)
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SOURCE_SIZE = mp.Vector3(physical_domains_size.x,physical_domains_size.y,0)
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NEAR_REGION_MONITOR_CENTER = mp.Vector3(0,0, DESIGN_REGION_UM.z + BUFFER/2)
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NEAR_REGION_MONITOR_SIZE = mp.Vector3(physical_domains_size.x,physical_domains_size.y,0)
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FF_MONITOR_CENTER = mp.Vector3(0,0,DESIGN_REGION_UM.z + BUFFER)
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FF_MONITOR_SIZE = mp.Vector3(DESIGN_REGION_UM.x, DESIGN_REGION_UM.y, 0)
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xs = ys = np.linspace(-FF_MONITOR_SIZE.x/2, FF_MONITOR_SIZE.x/2, NX_DESIGN_GRID)
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#collection of points in the far-field monitor
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ff_points = [mp.Vector3(x_p,y_p,FF_MONITOR_CENTER.z) for x_p in xs for y_p in ys]
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stop_cond = mp.stop_when_fields_decayed(25, mp.Ex, NEAR_REGION_MONITOR_CENTER, 1e-6)
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pml_layers = [mp.PML(PML_UM)]
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view_2D_plane = mp.Volume(
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center=mp.Vector3(0,0,0),
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size=mp.Vector3(cell_um.x,0,cell_um.z)
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)
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def str_from_list(list_: List[float]) -> str:
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return "[" + ", ".join(f"{val:.4f}" for val in list_) + "]"
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def obj_fun(epigraph_and_weights: np.ndarray, grad: np.ndarray)-> float:
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'''Objective function for the epigraph formulation
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Args:
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epigraph_and_weights: 1D array containing epigraph variable
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(at index 0) and design weigts (remaining elements)
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grad: the gradient modified in place of the objective function (flattened 1D array)
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Returns:
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The scalar epigraph variable (the objective function)
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'''
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epigraph = epigraph_and_weights[0]
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if grad.size > 0:
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grad[0] = 1
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grad[1:] = 0
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return epigraph
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def epigraph_constraint(
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result: np.ndarray,
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epigraph_and_weights: np.ndarray,
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gradient: np.ndarray,
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) -> None:
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'''Constraint function for the epigraph formulation
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Args:
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result: 1D array, modified in place, with the results
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of this constraint evaluation
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epigraph_and_weights: 1D array of epigraph (first element)
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and design weights (other elements)
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gradient: the jacobian matrix (backpropagated) with dimensions
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(1+NX_DESIGN_GRID*NY_DESIGN_GRID, 2 * num_wavelengths), modified in place.
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these gradients are used by the optimization algorithm,
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because, being backpropagated, they tell us how the constraint function behaves
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with respect to changes in the design parameters.
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sigmoid_threshold: erosion/dilation parameter for projection.
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sigmoid_bias: bias parameter for projection.
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use_epsavg: whether to use subpixel smoothing.
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'''
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print("Inside epigraph_constraint function...")
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epigraph = epigraph_and_weights[0]
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weights = epigraph_and_weights[1:]
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assert not np.isnan(weights).any(), "NaN values found in weights in epigraph_constraint function"
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print("===========")
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print("Shape of weights in epigraph_constraint:", weights.shape)
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print("===========")
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obj_val, grad = opt(
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[
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weights
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]
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)
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#modify in place the gradient result
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if gradient.size > 0:
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gradient[:,0] = -1 #gradient w.r.t epigraph
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gradient[:,1:] = grad.T
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#modify in place the constraint result
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result[:] = np.real(obj_val) - epigraph
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print("Updating history...")
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objfunc_history.append(np.real(obj_val))
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epivar_history.append(epigraph)
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print(
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f"iteration:, {cur_iter[0]:3d}, "
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f"epigraph: {epigraph:.5f}, obj. func.: {obj_val}, "
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f"epigraph constraint: {str_from_list(result)}"
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)
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print("Finished epigraph_constraint function")
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cur_iter[0] = cur_iter[0] + 1
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def get_pattern() -> np.ndarray:
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'''Imports the intensity pattern from file'''
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pattern_name = 'peg.png'
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pattern = Image.open('misc/' + pattern_name).convert('L')
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pattern = np.array(pattern).astype(float)
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pattern = pattern - np.min(pattern)
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pattern = pattern / np.max(pattern)
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return pattern
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def intensity_desired_fn_pattern(
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xs: list,
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ys: list,
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rescale: float = 0.5
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) -> np.ndarray:
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'''Returns the pattern intensity value at the specified
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(xs,ys) locations, with a scale factor
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Args:
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xs: list of x coordinates
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ys: list of y coordinates
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rescale: scale factor for the pattern
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Returns:
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The flattened pattern intensity value at the specified (xs,ys) locations, with a scale factor
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'''
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pattern_values = get_pattern()
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pattern_values = 1 - np.rot90(np.rot90(np.rot90(pattern_values)))
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nx,ny = pattern_values.shape
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xs_pattern = np.linspace(rescale*min(xs), rescale*max(xs), nx)
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ys_pattern = np.linspace(rescale*min(ys), rescale*max(ys), ny)
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pattern_dataArray = xr.DataArray(pattern_values, coords=dict(x=xs_pattern, y=ys_pattern))
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pattern_interp = pattern_dataArray.interp(x=xs, y=ys)
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pattern_final = npa.nan_to_num(pattern_interp.values, nan=npa.min(pattern_interp))
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pattern_to_return = npa.nan_to_num(pattern_interp.values, nan=npa.min(pattern_interp)).flatten()
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#make a plot before returning
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plt.figure()
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ax = plt.gca()
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im = ax.imshow(
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pattern_final,
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extent=(min(xs), max(xs), min(ys), max(ys)),
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origin='lower',
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cmap='inferno',
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)
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ax.set_xlabel('x (um)')
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ax.set_ylabel('y (um)')
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ax.set_title('Target Intensity Pattern')
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plt.colorbar(im, ax=ax, label='Intensity (a.u.)')
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plt.savefig("results/target_intensity_pattern.pdf")
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return pattern_to_return
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def normalization_sim() -> np.ndarray:
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''' Computes the Far-Field pattern at the monitor location and
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without the design region. Used for normalization purposes.
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Returns:
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A 2D-array [Nx*Ny,num_wavelengths] of reference intensities, for each wavelength,
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at the monitor location.
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'''
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sources = [
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mp.Source(
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src=mp.GaussianSource(
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frequency=frequency_center,
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fwidth=frequency_width
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),
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component=mp.Ex,
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center=SOURCE_CENTER,
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size=SOURCE_SIZE,
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)
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]
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substrate_block = mp.Block(
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center = SUBSTRATE_CENTER,
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size = SUBSTRATE_SIZE,
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material = SILICON_DIOXIDE,
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)
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geometry = [
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substrate_block,
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]
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norm_sim = mp.Simulation(
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resolution=RESOLUTION,
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default_material=AIR,
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cell_size=cell_um,
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sources=sources,
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geometry=geometry,
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boundary_layers=pml_layers,
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k_point=mp.Vector3(),
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)
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#plt.figure()
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#ax = plt.gca()
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#norm_sim.plot2D(output_plane=view_2D_plane, ax=ax)
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#plt.savefig("results/normalization_sim_setup.pdf")
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#plt.close()
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NearRegions = [mp.Near2FarRegion(
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center=NEAR_REGION_MONITOR_CENTER,
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size=NEAR_REGION_MONITOR_SIZE,
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weight=+1,
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)]
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norm_near2far = norm_sim.add_near2far(frequencies, *NearRegions)
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norm_sim.run(
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#mp.at_every(1,mp.in_volume(
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# mp.Volume(center=mp.Vector3(), size=physical_domains_size),
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# mp.output_efield_x
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#)),
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#mp.at_every(20,record_fields),
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until_after_sources=stop_cond
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)
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ref_fields = np.array(
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[norm_sim.get_farfield(norm_near2far, point) for point in ff_points]
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)
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#select only the (dft) Ex component for all frequencies,
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# which is the one we will optimize for
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ref_fields_x_f1 = ref_fields[:,0]
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ref_fields_x_f2 = ref_fields[:,6]
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ref_fields_x_f3 = ref_fields[:,12]
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#concatenate the Ex component for all frequencies into a single array
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#the rows are the points, the columns are the frequencies
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ref_fields_x = npa.stack((ref_fields_x_f1, ref_fields_x_f2, ref_fields_x_f3), axis=-1)
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ref_intensity_x = npa.power(npa.abs(ref_fields_x),2)
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#make a plot of the fields when simulation finished
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plt.figure()
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plt.subplot(1,3,1)
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plt.imshow(ref_intensity_x[:,0].reshape(NX_DESIGN_GRID, NY_DESIGN_GRID), extent=(min(xs), max(xs), min(ys), max(ys)), origin='lower')
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plt.title("Reference Intensity - 1.50 um")
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plt.xlabel("x (um)")
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plt.ylabel("y (um)")
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plt.colorbar(label='Intensity (a.u.)')
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plt.subplot(1,3,2)
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plt.imshow(ref_intensity_x[:,1].reshape(NX_DESIGN_GRID, NY_DESIGN_GRID), extent=(min(xs), max(xs), min(ys), max(ys)), origin='lower')
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plt.title("Reference Intensity - 1.55 um")
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plt.xlabel("x (um)")
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plt.ylabel("y (um)")
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plt.colorbar(label='Intensity (a.u.)')
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plt.subplot(1,3,3)
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plt.imshow(ref_intensity_x[:,2].reshape(NX_DESIGN_GRID, NY_DESIGN_GRID), extent=(min(xs), max(xs), min(ys), max(ys)), origin='lower')
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plt.title("Reference Intensity - 1.60 um")
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plt.xlabel("x (um)")
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plt.ylabel("y (um)")
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plt.colorbar(label='Intensity (a.u.)')
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plt.savefig("results/far_field_intensity_norm_sim.pdf")
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plt.close()
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return ref_intensity_x
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def intensity_from_farfields(FarFields) -> np.ndarray:
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'''Computes the intensity pattern at the monitor location from the simulated far-fields
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Args:
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FarFields: the simulated far-field patterns at the farfield
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monitor location, for each wavelength
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Returns:
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A 2D-array [Nx*Ny,num_wavelengths] of intensities, for each wavelength,
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at the monitor location.
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'''
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#select only the Ex component for all frequencies,
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# which is the one we will optimize for.
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#Reshape into matrix form (Nx,Ny)
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#print(FarFields.shape)
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#fields_x_f1 = FarFields[:,0,0].reshape(NX_DESIGN_GRID, NY_DESIGN_GRID)
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#fields_x_f2 = FarFields[:,1,0].reshape(NX_DESIGN_GRID, NY_DESIGN_GRID)
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#fields_x_f3 = FarFields[:,2,0].reshape(NX_DESIGN_GRID, NY_DESIGN_GRID)
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#concatenate the Ex component for all frequencies into a single array
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#the rows are the points, the columns are the frequencies
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#make a 3d arrray with dimensions (Nx,Ny,num_wavelengths)
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#fields_stack_3d = npa.stack((fields_x_f1, fields_x_f2, fields_x_f3), axis=-1)
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#fields_x = np.stack((fields_x_f1, fields_x_f2, fields_x_f3), axis=-1)
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intensity_x = npa.abs(FarFields[:,:,0]) ** 2
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return intensity_x
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def intensity_optimization(
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ref_intensity: np.ndarray,
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)-> mpa.OptimizationProblem:
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'''Sets up the optimization problem for the intensity pattern matching
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Args:
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ref_intensity: 2D array of reference intensities at the monitor location, for each wavelength
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use_damping: whether to use damping in the optimization algorithm
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use_epsavg: whether to use subpixel smoothing in the optimization
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sigmoid_bias: bias parameter for projection
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Returns:
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The optimization problem class instance
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'''
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matgrid = mp.MaterialGrid(
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grid_size = mp.Vector3(NX_DESIGN_GRID, NY_DESIGN_GRID,0),
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medium1 = AIR,
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medium2 = SILICON,
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weights = np.ones((NX_DESIGN_GRID, NY_DESIGN_GRID)),
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)
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matgrid_region = mpa.DesignRegion(
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matgrid,
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volume=mp.Volume(center=DESIGN_REGION_CENTER,
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size=DESIGN_REGION_UM
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)
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)
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matgrid_block = mp.Block(
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center=matgrid_region.center,
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size=matgrid_region.size,
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material=matgrid,
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)
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substrate_block = mp.Block(
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center = SUBSTRATE_CENTER,
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size = SUBSTRATE_SIZE,
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material = SILICON_DIOXIDE,
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)
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geometry = [
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matgrid_block,
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substrate_block,
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]
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sources = [
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mp.Source(
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src=mp.GaussianSource(frequency_center, fwidth=frequency_width),
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component=mp.Ex,
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size=SOURCE_SIZE,
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center=SOURCE_CENTER,
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)
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]
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sim = mp.Simulation(
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resolution=RESOLUTION,
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default_material=AIR,
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cell_size=cell_um,
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sources=sources,
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geometry=geometry,
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boundary_layers=pml_layers,
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k_point=mp.Vector3(),
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)
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NearRegions = [
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mp.Near2FarRegion(
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center=NEAR_REGION_MONITOR_CENTER,
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size=NEAR_REGION_MONITOR_SIZE,
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weight=+1,
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)
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]
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FarFields = mpa.Near2FarFields(
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sim=sim,
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Near2FarRegions=NearRegions,
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far_pts=ff_points,
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)
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obj_list = [FarFields]
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#2D array of target intensity at the monitor location
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target_intensity = intensity_desired_fn_pattern(xs, ys)
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target_intensity_3d = npa.tile(target_intensity[:,npa.newaxis], (1,num_wavelengths))
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target_intensity_mean = npa.mean(target_intensity)
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def J1(FarFields):
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'''Objective function. Computes the distance between simulated and target intensity patterns.
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Args:
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FarFields: the simulated far-field patterns at the monitor location, for each wavelength
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Returns:
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The distance between simulated and target intensity patterns
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'''
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measured_intensity = intensity_from_farfields(FarFields)
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#measured_intensity_mean = npa.mean(measured_intensity, axis=0)
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translated_measured_intensity = measured_intensity / npa.mean(ref_intensity,axis=0) * target_intensity_mean
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translated_measured_intensity = npa.clip(translated_measured_intensity, a_min=0, a_max=1)
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distance = translated_measured_intensity - target_intensity_3d
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distance_denominator = npa.full(target_intensity_3d.shape, 1)
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norm_distance = npa.power(npa.sum(distance**2, axis=0),0.5) / npa.power(npa.sum(distance_denominator**2, axis=0),0.5)
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return norm_distance
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opt = mpa.OptimizationProblem(
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simulation=sim,
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objective_functions=[J1],
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objective_arguments=obj_list,
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design_regions=[matgrid_region],
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frequencies=frequencies,
|
|
maximum_run_time=MAX_RUN_TIME
|
|
)
|
|
|
|
plt.figure()
|
|
ax = plt.gca()
|
|
opt.plot2D(True,output_plane=view_2D_plane, ax=ax)
|
|
plt.savefig("results/optimization_problem_setup.pdf")
|
|
|
|
return opt
|
|
|
|
if __name__ == "__main__":
|
|
print("Hello there! Starting normalization")
|
|
ref_intensity = normalization_sim()
|
|
|
|
num_weights = NX_DESIGN_GRID * NY_DESIGN_GRID
|
|
|
|
epigraph_and_weights = np.ones((num_weights,)) * 0.5
|
|
epigraph_and_weights = np.insert(epigraph_and_weights, 0, 1.2)
|
|
|
|
weights_lower_bound = np.zeros(num_weights)
|
|
weights_upper_bound = np.ones(num_weights)
|
|
epigraph_and_weights_lower_bound = np.insert(weights_lower_bound, 0, -np.inf)
|
|
epigraph_and_weights_upper_bound = np.insert(weights_upper_bound, 0, +np.inf)
|
|
|
|
objfunc_history = []
|
|
epivar_history = []
|
|
cur_iter = [0]
|
|
|
|
#max_evals = [48, 48, 60, 60, 60, 60]
|
|
max_evals = [5]*9
|
|
|
|
epigraph_tolerance = np.array([1e-4]*num_wavelengths)
|
|
|
|
for epoch, max_eval in enumerate(max_evals):
|
|
print(f"Starting optimization epoch {epoch} with max eval {max_eval}")
|
|
#the optimizer needs to work with the weights and epigraph (+1)
|
|
solver = nlopt.opt(nlopt.LD_CCSAQ, num_weights + 1)
|
|
solver.set_lower_bounds(epigraph_and_weights_lower_bound)
|
|
solver.set_upper_bounds(epigraph_and_weights_upper_bound)
|
|
solver.set_min_objective(obj_fun)
|
|
solver.set_maxeval(max_eval)
|
|
solver.set_param("dual_ftol_rel", 1e-7)
|
|
solver.add_inequality_mconstraint(
|
|
lambda result_, epigraph_and_weights_, grad_: epigraph_constraint(
|
|
result_,
|
|
epigraph_and_weights_,
|
|
grad_,
|
|
),
|
|
epigraph_tolerance,
|
|
)
|
|
solver.set_param("verbosity",1)
|
|
|
|
opt = intensity_optimization(
|
|
ref_intensity,
|
|
)
|
|
|
|
#execute a SINGLE forward run before the start of each epoch and
|
|
#manually set the initial epigraph variable to slightly larger
|
|
#than the largest value of the objective function over the
|
|
#wavelengths and the lengthscale constraint
|
|
#making a call to opt like the following invokes
|
|
#the __call__ method of the opt instance and starts the optimization
|
|
print("Calibrating epigraph variable before starting optimization...")
|
|
epigraph_initial, empty_grads = opt(
|
|
[
|
|
epigraph_and_weights[1:],
|
|
],
|
|
need_gradient=False,
|
|
)
|
|
#epigraph_initial contains the objective function values
|
|
#at each wavelength in the simulation. At each epoch,
|
|
#we set the initial epigraph variable taking the max of the objective functions
|
|
epigraph_and_weights[0] = np.max(epigraph_initial)
|
|
print(
|
|
f"epigraph-calibration: "
|
|
f"{str_from_list(epigraph_initial)}, {epigraph_and_weights[0]}"
|
|
)
|
|
|
|
print("Starting optimization...")
|
|
epigraph_and_weights[:] = solver.optimize(epigraph_and_weights)
|
|
print("Optimization completed")
|
|
|
|
optimal_design_weights = epigraph_and_weights[1:].reshape(-1, NY_DESIGN_GRID)
|
|
|
|
fig, ax = plt.subplots()
|
|
ax.imshow(
|
|
optimal_design_weights,
|
|
cmap="binary",
|
|
interpolation="none",
|
|
)
|
|
ax.set_axis_off()
|
|
if mp.am_master():
|
|
fig.savefig(
|
|
f"naive_design_epoch_{epoch}.png",
|
|
dpi=150,
|
|
bbox_inches="tight",
|
|
)
|
|
# Save the final (unmapped) design as a 2D array in CSV format
|
|
np.savetxt(
|
|
f"naive_design_weights_epoch_{epoch}.csv",
|
|
epigraph_and_weights[1:].reshape(NX_DESIGN_GRID, NY_DESIGN_GRID),
|
|
fmt="%4.2f",
|
|
delimiter=",",
|
|
)
|
|
|
|
plt.figure()
|
|
plt.subplot(1,2,1)
|
|
|
|
line1,line2,line3, = plt.plot(objfunc_history)
|
|
plt.xlabel("Iteration")
|
|
plt.ylabel("Value")
|
|
plt.legend([line1, line2, line3], ["Obj. func. - 1.50 um", "Obj. func. - 1.55 um", "Obj. func. - 1.60 um"])
|
|
|
|
plt.subplot(1,2,2)
|
|
plt.plot(epivar_history, label="Epigraph")
|
|
plt.xlabel("Iteration")
|
|
plt.ylabel("Value")
|
|
plt.legend()
|
|
|
|
plt.savefig(f"results/optimization_history_epoch_{epoch}.pdf")
|
|
|
|
saveResults = True
|
|
if saveResults:
|
|
with open('results/optimal_design.pkl', 'wb') as f:
|
|
pickle.dump({
|
|
'RESOLUTION': RESOLUTION,
|
|
'MAX_RUN_TIME': MAX_RUN_TIME,
|
|
'WAVELENGTH_MIN_UM': WAVELENGTH_MIN_UM,
|
|
'WAVELENGTH_MAX_UM': WAVELENGTH_MAX_UM,
|
|
'PML_UM': PML_UM,
|
|
'BUFFER': BUFFER,
|
|
'DESIGN_WAVELENGTHS_UM': DESIGN_WAVELENGTHS_UM,
|
|
'DESIGN_REGION_UM': DESIGN_REGION_UM,
|
|
'DESIGN_REGION_RESOLUTION': DESIGN_REGION_RESOLUTION,
|
|
'DESIGN_REGION_CENTER': DESIGN_REGION_CENTER,
|
|
'NX_DESIGN_GRID': NX_DESIGN_GRID,
|
|
'NY_DESIGN_GRID': NY_DESIGN_GRID,
|
|
'MIN_LENGTH_UM': MIN_LENGTH_UM,
|
|
'SILICON': SILICON,
|
|
'SILICON_DIOXIDE': SILICON_DIOXIDE,
|
|
'AIR': AIR,
|
|
|
|
'cell_um': cell_um,
|
|
|
|
'SUBSTRATE_THICKNESS': SUBSTRATE_THICKNESS,
|
|
'SUBSTRATE_SIZE': SUBSTRATE_SIZE,
|
|
'SUBSTRATE_CENTER': SUBSTRATE_CENTER,
|
|
|
|
'physical_domains_size': physical_domains_size,
|
|
|
|
'frequency_min': frequency_min,
|
|
'frequency_max': frequency_max,
|
|
'frequency_center': frequency_center,
|
|
'wavelength_center': wavelength_center,
|
|
'frequency_width': frequency_width,
|
|
'frequencies': frequencies,
|
|
'num_wavelengths': num_wavelengths,
|
|
|
|
'SOURCE_CENTER': SOURCE_CENTER,
|
|
'SOURCE_SIZE': SOURCE_SIZE,
|
|
|
|
'NEAR_REGION_MONITOR_CENTER': NEAR_REGION_MONITOR_CENTER,
|
|
'NEAR_REGION_MONITOR_SIZE': NEAR_REGION_MONITOR_SIZE,
|
|
|
|
'FF_MONITOR_CENTER': FF_MONITOR_CENTER,
|
|
'FF_MONITOR_SIZE': FF_MONITOR_SIZE,
|
|
'xs': xs,
|
|
'ys': ys,
|
|
'ff_points': ff_points,
|
|
|
|
|
|
'max_eval': max_eval,
|
|
'objfunc_history': objfunc_history,
|
|
'epivar_history': epivar_history,
|
|
'epigraph_variable': epigraph_and_weights[0],
|
|
'unmapped_design_weights': epigraph_and_weights[1:],
|
|
'optimal_design_weights': optimal_design_weights,
|
|
}, f)
|
|
|
|
print("Simulation completed")
|