mirror of
https://github.com/edoverg/modeconverter.git
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356 lines
10 KiB
Python
356 lines
10 KiB
Python
# %% [markdown]
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# This is a first attempt at creating an inverse designed fiber mode converter in meep. At first, we try to implement and combine tutorials from both tidy3d and meep.
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# %%
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import meep as mp
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import meep.adjoint as mpa
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import numpy as np
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from autograd import numpy as npa
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from autograd import tensor_jacobian_product, grad
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import nlopt
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from matplotlib import pyplot as plt
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from matplotlib.patches import Circle
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import scipy as sp
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import os
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# %%
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######PHYSICS SETUP######
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mp.verbosity(1)
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#setup a results folder
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if not os.path.exists("results"):
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os.makedirs("results")
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subs_index = 3.4
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subs_perm = subs_index**2
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Si = mp.Medium(index = subs_index)
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Air = mp.Medium(index = 1.0)
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wavelength = 1.55
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nf = 3 #number of frequencies to test
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frequencies = np.array([1/1.5, 1 / 1.55, 1 / 1.6])
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#distance between PML and source/monitor
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buffer = 2.5
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######PML######
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pml_size = 1.0
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pml_layers = [mp.PML(pml_size)]
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# %%
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######FILTER######
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minimum_length = 0.09 # minimum length scale (microns)
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eta_i = (
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0.5 # blueprint (or intermediate) design field thresholding point (between 0 and 1)
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)
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eta_e = 0.55 # erosion design field thresholding point (between 0 and 1)
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eta_d = 1 - eta_e # dilation design field thresholding point (between 0 and 1)
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filter_radius = mpa.get_conic_radius_from_eta_e(minimum_length, eta_e)
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# %%
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######DESIGN REGION######
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design_region_width = 4.0
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design_region_length = 4.0
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design_region_height = 1.0
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resolution = 15 # pixels/um
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design_region_resolution = int(resolution)
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#number of pixels in the design region
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Nx = int(design_region_width * design_region_resolution) + 1
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Ny = int(design_region_length * design_region_resolution) + 1
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design_variables = mp.MaterialGrid(mp.Vector3(Nx, Ny), Air, Si, grid_type="U_MEAN")
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design_region = mpa.DesignRegion(
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design_variables,
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volume=mp.Volume(
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center = mp.Vector3(0,0,design_region_height / 2),
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size = mp.Vector3(design_region_width,
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design_region_length,
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design_region_height),
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),
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)
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######CELL GEOMETRY######
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Sx = 2 * pml_size + design_region_width
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Sy = 2 * pml_size + design_region_length
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Sz = 2 * pml_size + design_region_height + 2*buffer
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print("Cell size: ", Sx, Sy, Sz)
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cell_size = mp.Vector3(Sx, Sy, Sz)
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substrate_thickness = Sz/2
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substrate_size = mp.Vector3(design_region_width, design_region_length, substrate_thickness)
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substrate_center = mp.Vector3(
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0,
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0,
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- substrate_thickness / 2)
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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 = Si,
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)
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design_region_block = mp.Block(
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center = design_region.center,
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size = design_region.size,
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material = design_variables,
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)
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geometry = [
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substrate_block,
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design_region_block,
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]
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# %%
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######SOURCE######
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fcen = 1 / wavelength
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width = 0.2
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fwidth = width * fcen
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source_center = [0, 0, -3]
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source_size = mp.Vector3(design_region_width, design_region_length, 0)
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src = mp.GaussianSource(frequency=fcen, fwidth=fwidth)
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source = [mp.Source(src, component=mp.Ex, size=source_size, center=source_center)]
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#src = mp.ContinuousSource(frequency=fcen, fwidth=fwidth, is_integrated=True)
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#source = [mp.Source(src, component=mp.Ex, size=source_size, center=source_center)]
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# %%
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######SIMULATION######
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kpoint = mp.Vector3()
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sim = mp.Simulation(
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cell_size = cell_size,
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boundary_layers = pml_layers,
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geometry = geometry,
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sources = source,
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default_material = Air,
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resolution = resolution,
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)
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# %%
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######MONITOR######
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far_field_obs_point_z_coord = 15
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far_z = [mp.Vector3(0,0,far_field_obs_point_z_coord)] #this is the far-field-focal-point
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NearRegions = [
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mp.Near2FarRegion(
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center=mp.Vector3(0,0, design_region_height + wavelength),
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size=mp.Vector3(design_region_width,design_region_length,0),
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weight=+1,
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)
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]
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#mpa.Near2FarFields return a numpy array with shape (num_of_points,nfreq,6) where the
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#third axis are the field components Ex,Ey,Ez,Hx,Hy,Hz
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FarFields = mpa.Near2FarFields(sim,NearRegions,far_z)
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ob_list = [FarFields]
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#this the objective to function
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#the objective is to maximize the obj function,
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def J1(FF):
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#in this case we want to maximize field intensity
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# at the position of the focal spot
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obj_to_return = npa.mean(npa.abs(FF[0,:,1]) ** 2)
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return obj_to_return
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#returns the first point of all frequencies of the Ey component
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# %%
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######CHECK PLOT######
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output_plane = mp.Volume(
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center=mp.Vector3(0,0,0),
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size=mp.Vector3(Sx-2*pml_size,0,Sz-2*pml_size))
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output_plane_xy = mp.Volume(
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center=mp.Vector3(0,0,design_region_height / 2),
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size=mp.Vector3(Sx-2*pml_size,Sy-2*pml_size,0)
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)
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fig = sim.plot2D(show_sources=True,show_monitors=True,show_epsilon=True, output_plane=output_plane)
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#sim.run(until=10)
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#sim.plot2D(fields=mp.Ex,output_plane=output_plane)
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#plt.savefig("fields.pdf")
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# %%
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######OPTIMIZATION PROBLEM######
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'''
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An OptimizationProblem class object knows how to do one basic thing:
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Given an input vector of design variables, compute the objective function value
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(forward calculation) and optionally its gradient (adjoint calculation)
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The gradient of the objective function is computed against its arguments, which are
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the FarFields.
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'''
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opt = mpa.OptimizationProblem(
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simulation=sim, #the optimizer uses this simulation object
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objective_functions=[J1], #the optimizer call this objective function
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objective_arguments=ob_list, #the optimizer passes this list of arguments to the objective function
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design_regions=[design_region], #the optimizer updates the design variables in this design region
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frequencies=frequencies, #the optimizer runs the simulation at these frequencies
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maximum_run_time=1500, #maximum optimizer run time
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)
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######CHECK PLOT######
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figure = opt.plot2D(True, output_plane=output_plane)
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# %%
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def mapping(x,eta,beta):
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'''
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Arguments:
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x: design variables (grey scale)
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eta: thresholding point for projection (between 0 and 1)
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beta: binarization strength for projection (positive)
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Returns:
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projected_field: the filtered and projected design variables
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'''
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#mapping is necessary to reach a physical design.
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#we start from the design variables (grey scale), which are values in the range (0,1).
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#typically, we set an initial value of 0.5.
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#filtering makes a local point behave more like its neighbourhood, avoiding checker patterns
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filtered_field = mpa.conic_filter(
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x,
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filter_radius,
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design_region_width,
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design_region_length,
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[design_region_resolution],
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)
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#projection
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#this is an hyperbolic tangent projection
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#after filtering, the design is still blurry, so we project it
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#using an tanh projection method to push the values towards the upper/lower bound
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#If a filtered value is >0.5, then we push it to 1, otherwise, if <0.5, we push it to 0.
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#parameter beta represents the degree of binarization,
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#parameter eta is threshold point
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projected_field = mpa.tanh_projection(filtered_field,beta,eta)
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#the following lines introduce symmetry. Need to understand if necessary
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#projected_field = (
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# npa.flipud(projected_field) + projected_field
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#)/2
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#interpolate to actual materials
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return projected_field.flatten()
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evaluation_history = []
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cur_iter = [0]
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def f(v, gradient, cur_beta):
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print("current iteration: {}".format(cur_iter[0]+1))
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#value and grad
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f0, dJ_du = opt([mapping(v,eta_i,cur_beta)])
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if gradient.size > 0:
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# NOTE: gradient is assigned in-place! No need to return.
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gradient[...] = tensor_jacobian_product(mapping, 0)(
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v, eta_i, cur_beta, np.sum(dJ_du, axis=1)
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)
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evaluation_history.append(np.real(f0))
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fig, (ax1, ax2) = plt.subplots(1, 2, figsize=(12, 5))
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opt.plot2D(
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False,
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ax=ax1,
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output_plane=output_plane,
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show_sources = False,
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show_monitors = False,
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show_boundary_layers = False,
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)
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circ1 = Circle((2,2), minimum_length/2)
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ax1.add_patch(circ1)
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opt.plot2D(
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False,
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ax=ax2,
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output_plane=output_plane_xy,
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show_sources = False,
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show_monitors = False,
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show_boundary_layers = False,
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)
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circ2 = Circle((2,2), minimum_length/2)
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ax2.add_patch(circ2)
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if not os.path.exists("results"):
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os.makedirs("results")
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plt.savefig("results/iter_{}.pdf".format(cur_iter[0]+1))
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cur_iter[0] += cur_iter[0] + 1
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return np.real(f0)
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algorithm = nlopt.LD_MMA
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n = Nx * Ny #number of parameters to optimize
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x = np.ones((n,)) * 0.5 #initial guess
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#x = np.insert(x, 0, -1)
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#lower and upper bounds for design variables
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lb = np.zeros((Nx * Ny,))
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ub = np.ones((Nx * Ny,))
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cur_beta = 4 #starting beta
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beta_scale = 2 #beta scaling (update) factor
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num_betas = 6 #number of betas to test
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update_factor = 12 #number of iterations per beta
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#total number of simulations = num_betas * update_factor * 2 (forward + adjoint)
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ftol = 1e-5
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optimization_start = True
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if optimization_start:
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for iters in range(num_betas):
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solver = nlopt.opt(algorithm, n)
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solver.set_lower_bounds(lb)
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solver.set_upper_bounds(ub)
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solver.set_max_objective(lambda v, g: f(v, g, cur_beta))
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solver.set_maxeval(update_factor) #number of iterations for each beta
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solver.set_ftol_rel(ftol)
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#observe that x is updated in place, so at
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# the end it will contain the optimized parameters
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x[...] = solver.optimize(x)
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cur_beta = cur_beta * beta_scale #update beta
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print("current beta: ", cur_beta)
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# %%
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######RESULTS######
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#plot the figure of merit over iterations
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plt.figure()
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plt.plot(evaluation_history)
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plt.xlabel("Iteration")
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plt.ylabel("Figure of Merit")
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plt.grid()
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plt.savefig("results/figure_of_merit.pdf")
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#plot and save the final design
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np.savetxt("results/final_design.txt", mapping(x, eta_i, cur_beta))
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opt.update_design([mapping(x, eta_i, cur_beta)])
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fig, (ax1, ax2) = plt.subplots(1, 2, figsize=(12, 5))
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opt.plot2D(
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False,
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ax=ax1,
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output_plane=output_plane,
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show_sources = False,
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show_monitors = False,
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show_boundary_layers = False,
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)
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circ1 = Circle((2,2), minimum_length/2)
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ax1.add_patch(circ1)
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ax1.axis("off")
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opt.plot2D(
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False,
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ax=ax2,
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output_plane=output_plane_xy,
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show_sources = False,
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show_monitors = False,
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show_boundary_layers = False,
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)
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circ2 = Circle((2,2), minimum_length/2)
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ax2.add_patch(circ2)
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ax2.axis("off")
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plt.savefig("results/final_design_xy.pdf") |