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Fourier relations in Optics

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A complex function f(t) may be decomposed ... Volume hologram. Volume grating. k1. k1. k1. k2. d. D. C. B. A. Bragg condition. d. D. C. B. A. Another example: ... – PowerPoint PPT presentation

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Title: Fourier relations in Optics


1
Fourier relations in Optics
Near field Far field
Frequency Pulse duration
Frequency Coherence length
Beam waist Beam divergence
Spatial dimension Angular dimension
Focal plane of lens The other focal plane
2
Huygens Principle
E(R)
E(r)
3
Fourier theorem A complex function f(t) may be
decomposed as a superposition integral of
harmonic function of all frequencies and complex
amplitude
(inverse Fourier transform) The component
with frequency ? has a complex amplitude F(?),
given by
(Fourier transform)
4
Useful Fourier relations in optics between t and
?, and between x and ?.


5
Useful Fourier relations in optics between t and
?, and between x and ?.
6
Position or time
Angle or frequency
7
Angle or frequency
Position or time
8
Single- slit diffraction
Application of Fourier relation
a
9
The applications of the Fourier relation
-Spatial harmonics and angles of propagation
10
?
11
Frequency, time, or position
12
N
w0
Time
Dw
Frequency
13
N
w0
Time
Dw
Frequency
Mode-locking
14
N
x0
Angle
Dx
Position
Diffraction grating, radio antenna array
15
The applications of the Fourier relation

(8)
Finite number of elements
16
-Graded grating for focusing -Fresnel lens
17
Fourier transform between two focal planes of a
lens
18
The use of spatial harmonics for analyses of
arbitrary field pattern
Consider a two-dimensional complex electric field
at z0 given by
where the ?s are the spatial frequencies in the
x and y directions.
The spatial frequencies are the inverse of the
periods.
19
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20
Thus by decomposing a spatial distribution of
electric field into spatial harmonics, each
component can be treated separately.
21
Define a transfer function (multiplication
factor) in free space for the spatial harmonics
of spatial frequency ?x and ?y to travel from z0
to zd as
22
Define a transfer function (multiplication
factor) in free space for the spatial harmonics
of spatial frequency ?x and ?y to travel from z0
to zd as
23
Source
E
E
z0
z0
24
To generalize
Grating momentum
25
Stationary gratings vs. Moving gratings
Deflection Frequency shift
Deflection
26
The small angle approximation (1/? ltlt?) for the H
function
???
A correction factor for the transfer function for
the plane waves
27
F(x)
H(?x)F(x)
D
z0
28
Express F(x,z) in ?x/z
29
Express F(x,z) in ?x/z
30
The effect of lenses

A lens is to introduce a quadratic phase shift to
the wavefront given by .
31
Fourier transform using a lens
32
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34
Huygens Principle
E(R)
E(r)
35
Recording of full information of an optical
image, including the amplitude and phase.
Holography
Amplitude only
Amplitude and phase
36
A simple example of recording and
reconstruction
?
k2
k1

37
A simple example of recording and
reconstruction
?
k2
k1

38

39
k2
k1
?/2

?
40
Another example Volume hologram
?
k2
k1

41
Volume grating

42
k1

43
k1
k2
k1

44
D
C
A
?
d
B
Bragg condition
45
D
C
A
?
d
B
46

Another example Image reconstruction of a point
illuminated by a plane wave.
Writing
47

Reading
48
E(x,y)
Er
Recorded pattern
49
Recorded pattern
Diffracted beam when illuminated by ER
50
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