Reanalysis for thesis (incl. plate scale change)

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yosata committed 2022-07-14 15:09:31 +02:00
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import numpy as np
import sys
# sys.path.insert(0, '/Users/joost/Dropbox/Werk/PhD/Analyses/Python/Analytical/Fourier Optics')
# sys.path.insert(0, '/home/joost/Dropbox/Werk/PhD/Analyses/Python/Analytical/Fourier Optics')
sys.path.insert(0, '/Users/joost/Dropbox/Werk/PhD/Documents/Published/FourierOptics GitHub release/')
from fourierOptics import *
from pdb import set_trace
'''
Author: Joost van den Born, PhD student at University of Groningen
Contact: born@astro.rug.nl
Description: Script to generate the geometric distortions due to WFEs
off the ADC prisms. The distortions are produced by measuring
the offset of the PSF centroid with and without WFE as a
function of field position.
Script made for the SPIE manuscript.
'''
def plot_distortions():
# Coordinates without WFEs
xe = load_variable('../data/GD_IFP_obscured_PSF_xcentroid_expected_zern.pkl')
ye = load_variable('../data/GD_IFP_obscured_PSF_ycentroid_expected_zern.pkl')
# Coordinates with WFEs
xf = load_variable('../data/GD_IFP_obscured_PSF_xcentroid_found_with_wfe_airy_zern.pkl')
yf = load_variable('../data/GD_IFP_obscured_PSF_ycentroid_found_with_wfe_airy_zern.pkl')
mcd = ParaxialMICADO(n=3001, m=3001, dpix=50, l=1.49e-3)
n = xe.shape[0]
X = xe.flatten()
Y = ye.flatten()
dX = xf - xe
dY = yf - ye
dx = dX.flatten()
dy = dY.flatten()
# Magnitude of the distortions
R = np.sqrt(dx**2 + dy**2) * mcd.platescale * 1e6
# Dummy figure, used for the colorbar colors in the quiver plot
im = plt.imshow(np.reshape(R, (n,n)))
plt.close()
fig = plt.figure()
ax = fig.add_subplot()
for i in range(len(xe)):
ax.plot(xe[:,i], ye[:,i], 'k-', alpha=0.2, linewidth=.5)
ax.plot(xe[i,:], ye[i,:], 'k-', alpha=0.2, linewidth=.5)
ax.quiver(X,Y,dx,dy, angles='xy', edgecolor='k', facecolor='None', linewidth=.5, units='dots')
ax.quiver(X,Y,dx,dy,R, alpha=.5, units='dots')
ax.set_aspect('equal', adjustable='box')
ax.set_xlabel('x (mm)')
ax.set_ylabel('y (mm)')
fig.colorbar(im, ax=ax, label='PSF centroid shift ($\\mu$as)')
plt.savefig('../figures/UPDATED_GD_focal_plane_zern.pdf', bbox_inches='tight', transparent=True)
plt.savefig('../figures/UPDATED_GD_focal_plane_zern.png', bbox_inches='tight', transparent=True)
plt.tight_layout()
plt.show()
if __name__ == '__main__':
# plt.rc('text', usetex=True)
# plt.rc('font', family='serif')
# Setup of simulation
l = 1.49e-3
mcd = ParaxialMICADO(n=3001, m=3001, dpix=50)
# mcd.plot_ray_trace()
wfe = WavefrontError(mcd.n, mcd.m)
# Get x3 and y3 (the coordinates to apply the ADC WFE to):
# The focal plane area is about 200x200 mm, so we apply the wavefront error to an area
# of 200x200 mm.
xfp, yfp = np.meshgrid(np.linspace(-150, 150, mcd.n), np.linspace(-150, 150, mcd.m))
# _, xfp, yfp = mcd.propagate(l=l,surface=1, zoom=False, show=False,
# print_progress=False)
# Generate a wavefront error for the intermediate focal plane.
print('\nSetting the wavefront errors...')
wfe_fp = WavefrontError(mcd.n,mcd.m)
wfe_rms = 50e-6
#PSD Wavefront error
# surface_map_fp = wfe_fp.generate_height_map(wfe_rms, 2, 1)
# plot_real_valued_results(surface_map_fp*1e6, xfp, yfp, logscale=False, fig_size=(8,6.4), grid=False, show=True,
# colormap='jet', labeltext='Surface height (nm)')
# save_variable('../data/MCD_IFP_wfe_object_PSD_50nm.pkl', wfe_fp)
# wfe_fp = load_variable('../data/MCD_IFP_wfe_object_PSD_50nm.pkl')
# surface_map_fp = wfe_fp.data
# Zernike wavefront error
# We re0se the ADC_surface classes because it can be applicable to any surface, if used properly
ifp_wfe = ADC_surfaces(xfp, yfp, clearAperture=300)
ifp_wfe.generate_ADC_wfe(zernRMS=wfe_rms, psdRMS=0.)
mask = np.sqrt(ifp_wfe.xz**2 + ifp_wfe.yz**2) > 1
# Plot the wfe
# surf_ifp = ifp_wfe.latest_surface.copy()
# surf_ifp[mask]=np.nan
# surface_map_fp = surf_ifp
# wfe_fp.data = surf_ifp
wfe_fp = load_variable('../data/MCD_IFP_wfe_object_zern_50nm.pkl')
surface_map_fp = wfe_fp.data
# save_variable('../data/MCD_IFP_wfe_object_zern_50nm.pkl', wfe_fp)
# figp1, axp1 = plot_real_valued_results(surface_map_fp*1e6, xfp, yfp,
# colormap='jet', labeltext='Surface height (nm)', fig_size=None, show=True)
plt.show()
Elist, Eplist = [], []
xlist, ylist = [], []
xplist, yplist = [], []
x_expected_list, y_expected_list = [], []
x_centroid_list, y_centroid_list = [], []
# Set field points
hxList, hyList = np.mgrid[-1:1:11j,-1:1:11j]-(1/300)
# hxList, hyList = np.mgrid[-.1/11:.1/11:11j,-.1/11:.1/11:11j]-(1/300) # Zoomed in to central area
hxList = hxList.flatten()
hyList = hyList.flatten()
# List of performed simulations
# Defined by PSD
## GD_IFP : -1:1
## GD_IFP_zoom : -1/11 :1/11
## GD_IFP_zoom2 : -.5/11:.5/11
## GD_IFP_zoom3 : -.1/11:.1/11
# Defined by zernikes
## GD_IFP_obscured_PSF_xcentroid_expected_zern : 50 nm rms 19 zernike modes : -1 : 1
## To do; check PSF shape at center field with zern wfe
## To do; check interpolated WFE at any zoomed in field point.
# Propagate through the field positions without any WFEs
for i in range(len(hxList)):
hx = hxList[i]
hy = hyList[i]
print('hx: {} - hy: {}'.format(hx,hy) )
# Initializing MICADO paraxial model
mcd = ParaxialMICADO(n=3001, m=3001, dpix=50, entrance_pupil='obscured')
# Propagate through the MICADO system
E, x, y = mcd.propagate(l=l,surface=-1, zoom=False, show=False,
print_progress=False, hx=hx, hy=hy)
# Find approximation for the centroid and amplitude as a first
# guess for the Obscured Airy pattern fit.
amplitude_guess = np.max(np.abs(E))**2
xbc, ybc, _, _ = mcd.centroid_shift(method='Barycenter')
print('Barycenter guess: ', xbc, ybc)
# Do the Obscured Airy Pattern Fit for the unperturbed PSF
xe, ye, _, _ = mcd.centroid_shift(method='Obscured Airy', initialGuess=(amplitude_guess, xbc, ybc, 0.0, 0.03))
print('Airy result: ', xe, ye)
x_expected_list.append(xe)
y_expected_list.append(ye)
# Load in the WFEs and set them to the corresponding ADC surfaces
print('\nSetting the wavefront errors...')
# null_wfe = np.zeros((3001,3001))
mcd.ELT_FP.add_wavefront_error(surface_map_fp, xfp, yfp, wfe=wfe_fp)
# Propagate through the MICADO system
print('Propagating with Wavefront Errors applied...')
Ep, xp, yp = mcd.propagate(l=l,surface=-1, zoom=False, show=False,
print_progress=False, hx=hx, hy=hy)
# Do the Obscured Airy Pattern Fit for the perturbed PSF
xf, yf, _, _ = mcd.centroid_shift(method='Obscured Airy', initialGuess=(amplitude_guess, xe, ye, 0.0, 0.03))
# Resulting centroid shift due to the WFE
x_centroid_list.append(xf)
y_centroid_list.append(yf)
R = np.sqrt( (xf-xe)**2 + (yf-ye)**2 ) * mcd.platescale * 1e6
print('xf: {}, yf: {}, shift (uas): {}'.format(xf,yf, R))
# Clear the memory by emptying the large arrays
mcd = None
wfe = None
E, x, y = None, None, None
Ep, xp, yp = None, None, None
# Reshaping the arrays
shape = (int(np.sqrt(len(x_expected_list))), int(np.sqrt(len(x_expected_list))))
x_expected = np.asarray(x_expected_list).reshape(shape)
y_expected = np.asarray(y_expected_list).reshape(shape)#.T
# Saving the arrays
save_variable('../data/GD_IFP_obscured_PSF_xcentroid_expected_zern.pkl', x_expected)
save_variable('../data/GD_IFP_obscured_PSF_ycentroid_expected_zern.pkl', y_expected)
# Reshaping the arrays
shape = (int(np.sqrt(len(x_centroid_list))), int(np.sqrt(len(x_centroid_list))))
x_centroid = np.asarray(x_centroid_list).reshape(shape)
y_centroid = np.asarray(y_centroid_list).reshape(shape)
# Saving the arrays
save_variable('../data/GD_IFP_obscured_PSF_xcentroid_found_with_wfe_airy_zern.pkl', x_centroid)
save_variable('../data/GD_IFP_obscured_PSF_ycentroid_found_with_wfe_airy_zern.pkl', y_centroid)
plot_distortions()