Holography and Faraday Rotation Fourier Optics
Transcript of Holography and Faraday Rotation Fourier Optics
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Holography and Faraday Rotation Fourier Optics
Please turn in your late reports to TAs
Wednesday: Veteran’s day. The make up lab will be the Wednesday of the Thanks Giving week.
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Fourier Analysis
Fourier series for periodic functions:
Hecht, Pg 304
Fourier’s Theorem: a function f(x), having a spatial period λ, can be synthesized by a sum of harmonic functions whose wavelengths are integral of submultiples of λ.
0
0 0
( ) cos( ) sin( )2
m m
Af x A mkx B mkx
0
2( )cos( )mA f x mkx dx
0
2( )sin( )mB f x mkx dx
k=2π/ λ
Determine A and B through Fourier analysis.
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Holograms: Fourier Optics
Hecht pg 626, fig. 13.45
1960, Leith & Upatnieks @ U. Michigan
Making holograms
Reconstruct wavefront
mirror
Coherent reference wave
Scattered light
Photo plate
Virtual image
What does standard photograph do?
Dennis Gabor
Key Idea – record interference patternbetween object beam and reference beam
Recording amplitudeand phase of light field. Gives “3D” picture.
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Holograms: Fourier Optics
Hecht pg 626, fig. 13.45
Recording amplitudeand phase of light field. Gives “3D” picture.
Key Idea – record interference patternbetween object beam and reference beam
1960, Leith & Upatnieks @ U. Michigan
Making holograms
Reconstruct wavefront
mirror
Coherent reference wave
Scattered light
Photo plate
Virtual image
Dennis Gabor
![Page 5: Holography and Faraday Rotation Fourier Optics](https://reader034.fdocuments.in/reader034/viewer/2022051510/627e8c398b26220d43557e78/html5/thumbnails/5.jpg)
What does standard photograph do?
Hololens
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Standard photographs – only record intensity distribution of light.
Holography, Fourier transform between real image to spatial frequency domain. Spatial frequency of the objective is recorded by the film-> hologram. Fourier transform of the hologram reconstruct the object.
Holograms: Fourier Optics
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Hecht pg 628, fig. 13.48Reference wave
Object wave
H
A
B
C
A
B
λ
θ
sinAB
A Simple View of Hollogram
x
( )
2
x x
AB
( ) 2 sin( ) /
sin( )
x x
kx
If intensity is correct, a cosine (sine) gratingis produced with diffraction peaks 0, +/- 1 only
The intensity distribution on the plane
( ) (1 cos )oI x I
A cosine grating is created with spatial period of AB .
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Hologram ofCosine Grating
Record
Playback
Three diffracted waves
The amplitude of the object wave at every point on the film plane will be encoded in the visibility of the resulting fringes.
Complicated object -> complicated fringe pattern and contrast
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Question: In the hologram, where is the phase information stored?And where is the intensity information stored?
Hologram: record both intensity and phase information.
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Question: In the hologram, where is the phase information stored? (fringe pattern)
And where is the intensity information stored? (fringe contrast)
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If we block most of the hologram and only leave part of it illuminated by the reconstructed wave, can we observe the whole object and why?
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If yes, what is the difference compared to illuminating the whole hologram?
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Photographic Film Response
G determines contrast and is related to film speed
Characteristic response curve
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Diffraction Grating generated using Holography
Beam Splitter
MirrorPhotographic plate
Record the grating Using the grating
Because a holographic diffraction grating has no periodic errors or imperfections, it exhibits significantly lower stray light compared to a ruled grating
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y
z
Diffraction Grating generated using Holography
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Diffraction Grating generated using Holography
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Diffraction Grating generated using Holography