Interferometric measurement of rotationally symmetric aspheric ...
Nasrin Ghanbari OPTI 521. Introduction Spherical wavefront from interferometer is incident on CGH...
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Transcript of Nasrin Ghanbari OPTI 521. Introduction Spherical wavefront from interferometer is incident on CGH...
![Page 1: Nasrin Ghanbari OPTI 521. Introduction Spherical wavefront from interferometer is incident on CGH Reflected light will have an aspheric phase function.](https://reader033.fdocuments.net/reader033/viewer/2022051214/56649c9d5503460f9495c39d/html5/thumbnails/1.jpg)
Using CGH for Testing Aspheric Surfaces
Nasrin GhanbariOPTI 521
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IntroductionSpherical wavefront from
interferometer is incident on CGH
Reflected light will have an aspheric phase function
CGH cancels the aspheric phase
Emerging wavefront will be spherical and it goes back to interferometer
CGH
Aspheric Mirror
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Design Process
Start with design and optimization of CGH in Zemax:Single pass geometryPhase functionDouble pass geometry
Design of CGH in Zemax
Alignment CGH
Conversion to line pattern
Fabrication
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Virtual GlassSnell’s law:
If n1 = 0 then sin θ2 =0
Therefore θ2 =0 and the emerging ray is perpendicular to aspheric surface
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Single Pass Geometry
CGH
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Beam Footprint Width of the spot
size:
The number of waves of tilt needed to separate diffraction orders:
[1]
A p e r t u r e D i a m e t e r : 4 . 8 8 6 1
Scale: 5.0000 Millimeters
d T _ C G H _ I l l u m i n a t i o n _ I I . Z M XC o n f i g u r a t i o n 1 o f 1
F o o t p r i n t D i a g r a m
1 2 / 1 / 2 0 1 2S u r f a c e 2 0 : R a y X M i n = - 0 . 3 8 7 2 R a y X M a x = 0 . 3 8 7 2R a y Y M i n = - 2 . 4 4 3 1 R a y Y M a x = 1 . 1 9 4 0M a x R a d i u s = 2 . 4 4 3 1 W a v e l e n g t h = 0 . 6 3 2 8
% r a y s t h r o u g h = 1 0 0 . 0 0 %
[1] Dr. Jim Burge, “Computer Generated Holograms for Optical Testing”
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Phase Design
ZernikeCoefficient Value
ZernikeCoefficient Value
ZernikeCoefficient Value
A 1 0.00E+00 A 13 3.85E-04 A 25 -9.49E-03A 2 1.10E+02 A 14 6.89E-05 A 26 0.00E+00A 3 0.00E+00 A 15 -2.50E+00 A 27 -7.18E-01A 4 -3.27E+01 A 16 -3.94E-01 A 28 -2.89E-01A 5 7.00E+01 A 17 -3.07E+00 A 29 -4.89E-05A 6 -1.74E-01 A 18 -8.31E-05 A 30 -1.80E-05A 7 -6.57E-02 A 19 -3.30E-05 A 31 7.30E-02A 8 -2.89E+01 A 20 1.60E+00 A 32 6.16E-03A 9 -4.41E+00 A 21 6.22E-01 A 33 2.35E-05A 10 -4.13E-04 A 22 1.06E-04 A 34 2.06E-06A 11 1.24E+01 A 23 -3.56E-06 A 35 -4.81E-03A 12 6.26E+00 A 24 -1.76E-01 A 36 5.94E-04
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Zernike Fringe Phase
M is the diffraction order of the CGHN is the number of Zernike terms; Zemax
supports up to 37Zi (ρ,φ) is the ith term in the Zernike polynomial
Ai is the coefficient of that term in units of waves.
Ai Zi (ρ,φ)
A1 1
A2 ρ cos(φ)
A3 ρ sin(φ)
A4 2 ρ2 - 1
A5 ρ2cos (2 φ)
A6 ρ2 sin(2 φ)...
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Double Pass Geometry
The double pass geometry models the physical setup.Check the separation of various diffraction ordersFlip the sign of diffraction order for CGH and radius
of curvature for the mirror
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Diffraction Orders
A p e r t u r e D i a m e t e r : 1 0 . 0 0 0 0
Scale: 10.2000 Millimeters
g T _ D P _ D i f f r a c t i o n _ O r d e r s . Z M XC o n f i g u r a t i o n : A l l 7
F o o t p r i n t D i a g r a m
1 2 / 2 / 2 0 1 2S u r f a c e 1 1 : B e s t F o c u s V o r w a r dR a y X M i n = - 5 . 4 4 2 8 R a y X M a x = 3 . 5 6 5 0R a y Y M i n = - 3 . 7 5 1 9 R a y Y M a x = 8 . 5 5 7 8M a x R a d i u s = 1 0 . 0 3 6 7 W a v e l e n g t h = 0 . 6 3 2 8
% r a y s t h r o u g h = 7 5 . 7 5 %
( a )
A p e r t u r e D i a m e t e r : 1 0 . 0 0 0 0Scale: 10.2000 Millimeters
g T _ D P _ D i f f r a c t i o n _ O r d e r s . Z M XC o n f i g u r a t i o n : A l l 7
F o o t p r i n t D i a g r a m
1 2 / 2 / 2 0 1 2S u r f a c e 2 1 : B e s t F o c u s R e t u r nR a y X M i n = - 3 . 0 4 9 5 R a y X M a x = 5 . 7 5 1 6R a y Y M i n = - 6 . 7 3 8 4 R a y Y M a x = 5 . 5 1 6 6M a x R a d i u s = 8 . 8 1 0 5 W a v e l e n g t h = 0 . 6 3 2 8
% r a y s t h r o u g h = 7 5 . 7 5 %
( b )
Use multi-configuration editor in Zemax The +1 diffraction order appears in redTo block other orders place an aperture at best
focus.
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Sources of ErrorPattern Distortion:
error in the positioning of the fringe linesMisalignment of CGH:
alignment marks and cross hairs are placed around the main CGH
[2] R. Zehnder, J. Burge and C. Zhao, “Use of computer generated holograms for alignment of complex null correctors”
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2D Line Pattern
Ph
ase
F
un
ctio
n
Position on Substrate
Wavefront Profile [1]
Chrome Segment
Spacing
[1] Dr. Jim Burge, “Computer Generated Holograms for Optical Testing”
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Physical Setup
CGH
*Photos taken at the Mirror Lab
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ConclusionPhase function of CGH can be optimized for a
particular testing geometry.The process is carried out in three stepsTilt must be added to CGH to separate +1
order from the other diffraction orders.Diffraction efficiency was not discussed; for an
amplitude grating it is about 10% for the +1 order
For accurate placement of CGH in the testing setup, it is necessary to include the alignment CGH.
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Thank You Chunyu ZhaoDaewook KimJavier Del HoyoTodd HorneWenrui CaiWon Hyun Park