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docs/_downloads/722a8375241f5baec2512e3d683cd39b/Michelson-with-lens.py
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#! /usr/bin/env python | ||
from LightPipes import * | ||
import matplotlib.pyplot as plt | ||
|
||
wavelength=632.8*nm #wavelength of HeNe laser | ||
size=15*mm # size of the grid | ||
N=500 # number (NxN) of grid pixels | ||
R=9*mm # laser beam radius | ||
z1=8*cm # length of arm 1 | ||
z2=7*cm # length of arm 2 | ||
z3=3*cm # distance laser to beamsplitter | ||
z4=5*cm # distance beamsplitter to screen | ||
Rbs=0.5 # reflection beam splitter | ||
tx=0.0*mrad; ty=0.0*mrad # tilt of mirror 1 | ||
f_lens = 500*cm | ||
|
||
#Generate a laser beam: | ||
F=Begin(size,wavelength,N) | ||
F=GaussBeam(F, R) | ||
|
||
#Propagate to the beamsplitter: | ||
F=Forvard(z3,F) | ||
|
||
#Split the beam and propagate to mirror #2: | ||
F2=IntAttenuator(1-Rbs,F) | ||
F2=Forvard(z2,F2) | ||
|
||
#Introduce aberration and propagate back to the beamsplitter: | ||
F2=Tilt(tx,ty,F2) | ||
F2 = Lens(f_lens, F2) | ||
F2=Forvard(z2,F2) | ||
F2=IntAttenuator(Rbs,F2) | ||
|
||
#Split off the second beam and propagate to- and back from the mirror #1: | ||
F10=IntAttenuator(Rbs,F) | ||
F1=Forvard(z1*2,F10) | ||
F1=IntAttenuator(1-Rbs,F1) | ||
|
||
#Recombine the two beams and propagate to the screen: | ||
F=BeamMix(F1,F2) | ||
F=Forvard(z4,F) | ||
I=Intensity(1,F) | ||
|
||
s1 = r'LightPipes for Python ' + LPversion + '\n\n'\ | ||
r'Michelson interferometer with a lens in one arm' + '\n' | ||
s2 = r'Michelson.py'+ '\n\n'\ | ||
f'size = {size/mm:4.2f} mm' + '\n'\ | ||
f'$\\lambda$ = {wavelength/um:4.2f} $\\mu$m' + '\n'\ | ||
f'N = {N:d}' + '\n'\ | ||
f'R = {R/mm:4.2f} mm beam radius of the laser' + '\n'\ | ||
f'z1 = {z1/mm:4.2f} mm length of arm 1' + '\n'\ | ||
f'z2 = {z2/mm:4.2f} mm length of arm 2' + '\n'\ | ||
f'z3 = {z3/mm:4.2f} mm distance from the laser to the beam splitter' + '\n'\ | ||
f'z4 = {z4/mm:4.2f} mm distance from the beam splitter to the screen' + '\n'\ | ||
f'tx, ty = {tx/mrad:4.2f}, {ty/mrad:4.2f} mrad tilt of mirror 2' + '\n'\ | ||
r'$f_{lens}$ = ' + f'{f_lens/cm:4.2f} cm focal length of the lens in arm 2' + '\n\n'\ | ||
r'${\copyright}$ Fred van Goor, June 2020' | ||
|
||
fig=plt.figure(figsize=(6,9)); | ||
ax1 = fig.add_subplot(311);ax1.axis('off') | ||
ax2 = fig.add_subplot(312);ax2.axis('off') | ||
ax3 = fig.add_subplot(313);ax3.axis('off') | ||
ax1.imshow(I,cmap='jet');ax1.set_title('intensity pattern') | ||
ax2.text(0.0,0.6,s1,fontsize=12, fontweight='bold') | ||
ax3.text(0.0,0.50,s2) | ||
|
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plt.show() |
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docs/_downloads/ae71177a83317cd5339787a1561145ad/Michelson-with-aberration.py
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#! /usr/bin/env python | ||
from LightPipes import * | ||
import matplotlib.pyplot as plt | ||
|
||
wavelength=632.8*nm #wavelength of HeNe laser | ||
size=15*mm # size of the grid | ||
N=500 # number (NxN) of grid pixels | ||
R=9*mm # laser beam radius | ||
z1=8*cm # length of arm 1 | ||
z2=7*cm # length of arm 2 | ||
z3=3*cm # distance laser to beamsplitter | ||
z4=5*cm # distance beamsplitter to screen | ||
Rbs=0.5 # reflection beam splitter | ||
tx=0.0*mrad; ty=0.0*mrad # tilt of mirror 1 | ||
zernabb = 7 # Zernike aberration (7 = vertical coma) | ||
|
||
|
||
|
||
#Generate a laser beam: | ||
F=Begin(size,wavelength,N) | ||
F=GaussBeam(F, R) | ||
|
||
#Propagate to the beamsplitter: | ||
F=Forvard(z3,F) | ||
|
||
#Split the beam and propagate to mirror #2: | ||
F2=IntAttenuator(1-Rbs,F) | ||
F2=Forvard(z2,F2) | ||
|
||
#Introduce aberration and propagate back to the beamsplitter: | ||
F2=Tilt(tx,ty,F2) | ||
(mz, nz) = noll_to_zern(zernabb) | ||
F2=Zernike(F2, mz, nz, 6*mm, A=1.03*wavelength) | ||
F2=Forvard(z2,F2) | ||
F2=IntAttenuator(Rbs,F2) | ||
|
||
#Split off the second beam and propagate to- and back from the mirror #1: | ||
F10=IntAttenuator(Rbs,F) | ||
F1=Forvard(z1*2,F10) | ||
F1=IntAttenuator(1-Rbs,F1) | ||
|
||
#Recombine the two beams and propagate to the screen: | ||
F=BeamMix(F1,F2) | ||
F=Forvard(z4,F) | ||
I=Intensity(1,F) | ||
|
||
s1 = r'LightPipes for Python ' + LPversion + '\n\n'\ | ||
r'Michelson interferometer with Zernike'+ '\n' + 'aberration in one arm' + '\n' | ||
|
||
s2 = r'Michelson-with-aberration.py'+ '\n\n'\ | ||
f'size = {size/mm:4.2f} mm' + '\n'\ | ||
f'$\\lambda$ = {wavelength/um:4.2f} $\\mu$m' + '\n'\ | ||
f'N = {N:d}' + '\n'\ | ||
f'R = {R/mm:4.2f} mm beam radius of the laser' + '\n'\ | ||
f'z1 = {z1/mm:4.2f} mm length of arm 1' + '\n'\ | ||
f'z2 = {z2/mm:4.2f} mm length of arm 2' + '\n'\ | ||
f'z3 = {z3/mm:4.2f} mm distance from the laser to the beam splitter' + '\n'\ | ||
f'z4 = {z4/mm:4.2f} mm distance from the beam splitter to the screen' + '\n'\ | ||
f'tx, ty = {tx/mrad:4.2f}, {ty/mrad:4.2f} mrad tilt of mirror 2' + '\n'\ | ||
f'Zernike aberration = {noll_to_zern(zernabb)}, {ZernikeName(zernabb)}' + '\n\n'\ | ||
r'${\copyright}$ Fred van Goor, June 2020' | ||
|
||
fig=plt.figure(figsize=(6,9)); | ||
ax1 = fig.add_subplot(311);ax1.axis('off') | ||
ax2 = fig.add_subplot(312);ax2.axis('off') | ||
ax3 = fig.add_subplot(313);ax3.axis('off') | ||
ax1.imshow(I,cmap='jet');ax1.set_title('intensity pattern') | ||
ax2.text(0.0,0.6,s1,fontsize=12, fontweight='bold') | ||
ax3.text(0.0,0.50,s2) | ||
|
||
plt.show() |
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