professor j. gopinath - university of colorado...
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Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
ECEN 4606Undergraduate Optics Lab
Interferometry
Professor J. Gopinath
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Administrative Details• Prelab #4 due now!• CU Learn ?, either 0 or 10 points
- Credit for completion• Lab #1
- average was 80- can drop one lab score
• Handout: Lab #5 and Lecture #6• Prelab redos
- Turn in by time lab report is due• MATLAB required for Prelab #5
- Access1. EECS Shell2. SRC3. Office hours4. Access to ECEE 282
Buff card activated at front deskLab access EXCEPT following times:
Tues: 8 – 10 am, 12 – 2 pm, 6-8 pmWed: 3 – 5 pmThurs: 10 am – 3 pm
5. ITS Labs in Engineering
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Fringe Visibility
Hecht, Optics, p. 561
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Interference: Spherical Waves
• Professor McLeod, CU-Boulder
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Spherical Aberration4
040ρWW =∆
Wavefront error in pupilW040 = 1
Interferogram
-1
-0.5
0
0.5
1 -1
-0.5
0
0.5
1
-4
-3
-2
-1
0
-1
-0.5
0
0.5
1
W∆
xy
y
x• Professor McLeod, CU-Boulder• Wyant and Creath, Basic WavefrontAberration Theory for Optical Metrology
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Coma
20131
30131 cos ρθρ xxWxWW ==∆
Wavefront error in pupilW131 = 1
-1
-0.5
0
0.5
1 -1
-0.5
0
0.5
1
-2
-1
0
1
2
-1
-0.5
0
0.5
1
W∆
x
y
x
y
• Professor G. Yoon, University of Rochester, Aberration Theory •Professor McLeod, CU-Boulder
Interferogram
Coma is absent on axis, and increases with field angle
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Astigmatism
220222
2220222 cos xxWxWW ==∆ θρ
Wavefront error in pupilW222 = 1
-1
-0.5
0
0.5
1 -1
-0.5
0
0.5
1
-1
-0.75
-0.5
-0.25
0
-1
-0.5
0
0.5
1
W∆
x
y
x
y
Interferogram
• Professor McLeod, CU-Boulder• Professor G. Yoon, University of Rochester, Aberration Theory
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Field Curvature
220220 ρxWW =∆
Wavefront error in pupilW220 = 1
-1
-0.5
0
0.5
1 -1
-0.5
0
0.5
1
-2
-1.5
-1
-0.5
0
-1
-0.5
0
0.5
1
W∆
x
y
x
y
• Professor McLeod, CU-Boulder•Professor G. Yoon, University of Rochester, Aberration Theory
Interferogram
Image appears on curved surface
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Distortion
xxWxWW 30311
30311 cos ==∆ θρ
Wavefront error in pupilW311 = 1
-1
-0.5
0
0.5
1 -1
-0.5
0
0.5
1
-1
-0.5
0
0.5
1
-1
-0.5
0
0.5
1
W∆
x
y
x
y
Interferogram
• Professor McLeod, CU-Boulder• Wyant and Creath, Basic Wavefront Aberration Theory for Optical Metrology
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Summary of aberrations
Wyant and Creath, Basic WavefrontAberration Theory for Optical Metrology
The spatial coherence length is the transverse distance over which the beam wave-fronts remain flat:
The temporal coherence time and the spatial coherence lengthThe temporal coherence time is how long the beam remains sinusoidal at a single wavelength:
Since there are two transverse dimensions, we can define a spatial
coherence area, Ac.
Temporal Coherence
Time, τc
Spatial Coherence
Length, xc
τc
Wave-fronts
xc
k
k
Wave-fronts
Trebino, Georgia Tech, UG optics course
Spatial and Temporal Coherence
Beams can be coherent or
only partially coherent
(indeed, even incoherent)
in both space and time.
Spatial andTemporal
Coherence:
TemporalCoherence;
Spatial Incoherence
Spatial Coherence;
TemporalIncoherence
Spatial andTemporal
Incoherence
xc
τc
τc
Wave-fronts
τc
τc
xc
xc
xc
Trebino, Georgia Tech, UG optics course
How quickly will a light wave deviate from a perfect sine wave in time?
0 21 21 0exp exp ( )( , ) Re{ }( )tot E i k xE E i k x tx tt ωω−= −+
So the phase will drift on a time scale of: ~ 2π/∆ω = 1/∆ν
Suppose the light wave has two frequencies:
τ
Ε
The two frequencies will become significantly out of phase with each other in a time, tc:
2
2
1
1
22 / ( )
c c
c
τ τ πτ ωπ
ω ωω
− =⇒ = −
1 2 2ω π νωω∆ = − = ∆where:Trebino, Georgia Tech, UG optics course
The coherence time is the reciprocal of the bandwidth.
The largest frequency difference in the light wave will yield the shortest phase-drift time, which we call the coherence time:
1/c vτ = ∆
where Dn is the light bandwidth (the width of the spectrum).
Sunlight and light bulbs are temporally very incoherent—and have very small coherences times (a few fs)—because their bandwidths are very large (the entire visible spectrum).
Lasers can have much longer coherence times—as long as about a second, which is amazing; that's >1014 cycles!
Trebino, Georgia Tech, UG optics course
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Astigmatism at Circle of Least Confusion
Wavefront error in pupilW222 = 1
Interferogram
-1
-0.5
0
0.5
1 -1
-0.5
0
0.5
1
-0.5
-0.25
0
0.25
0.5
-1
-0.5
0
0.5
1
W∆
x
y
x
y
( ) ( )2212
212
02222
21222
0222 cos yxxWxWW −=−=∆ ρθρ
• Professor McLeod, CU-Boulder• Wyant and Creath, Basic Wavefront Aberration Theory for Optical Metrology
Professor J. GopinathUniversity of Colorado at Boulder
ECEN 4606, Undergraduate Optics Lab
Spherical aberration at Circle of Least Confusion
( )2234
040 ρρ −=∆ WW
Wavefront error in pupilW040 = 1
Interferogram
-1
-0.5
0
0.5
1 -1
-0.5
0
0.5
1
-1
-0.5
0
0.5
-1
-0.5
0
0.5
1
W∆
x
y
x
y
• Professor McLeod, CU-Boulder