Download - Matrix methods, aberrations optical systems
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Matrix methods, aberrations & optical systemsFriday September 27, 2002
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System matrix
o
o
f
f yDCBAy
oof
oof
DCy
BAyy
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System matrix: Special Cases(a) D = 0 (a) D = 0 ff = Cy = Cyo o (independent of (independent of oo))
yyoo
ff
Input plane is the first focal planeInput plane is the first focal plane
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System matrix: Special Cases(b) A = 0 (b) A = 0 y yff = B = Boo (independent of y (independent of yoo))
oo
yyff
Output plane is the second focal planeOutput plane is the second focal plane
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System matrix: Special Cases(c) B = 0 (c) B = 0 y yff = Ay = Ayoo
yyff
Input and output plane are conjugate – A = magnificationInput and output plane are conjugate – A = magnification
yyoo
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System matrix: Special Cases(d) C = 0 (d) C = 0 ff = D = Doo (independent of y (independent of yoo))
Telescopic system – parallel rays in : parallel rays outTelescopic system – parallel rays in : parallel rays out
oo ff
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Examples: Thin lens
L
LL
nPd
nn
nP
nnd
nPd
TL2
1
12
1''
1
Recall that for a thick lensRecall that for a thick lens
For a thin lens, d=0For a thin lens, d=0
''
01
nn
nPL
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Examples: Thin lens
LnPPdPPP 21
21
'''
2121 f
nfn
Rnn
RnnPPP LL
Recall that for a thick lensRecall that for a thick lens
For a thin lens, d=0For a thin lens, d=0
In air, n=n’=1In air, n=n’=1
2121
11111'
11RR
nRn
Rn
ffP L
LL
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Imaging with thin lens in air
oo’’
ss s’s’
yyoo y’y’
Input Input
planeplaneOutput Output planeplane
11
01
fL
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Imaging with thin lens in air
)()'( sTLsTS
101
10'1 s
DCBAs
S
DCsC
DsCssBAsCsADCBA '''
''''
For thin lens: For thin lens: A=1A=1 B=0B=0 D=1D=1 C=-1/f C=-1/f
y’ = A’yy’ = A’yoo + B’ + B’oo
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Imaging with thin lens in air
y’ = A’yy’ = A’yoo + B’ + B’oo
For imaging, y’ must be independent of For imaging, y’ must be independent of oo
B’ = 0B’ = 0
B’ = As + B + Css’ + Ds’ = 0B’ = As + B + Css’ + Ds’ = 0
s + 0 + (-1/f)ss’ + s’ = 0s + 0 + (-1/f)ss’ + s’ = 0
For thin lens: For thin lens: A=1A=1 B=0B=0 D=1D=1 C=-1/f C=-1/f
fss1
'11
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Examples: Thick Lens
nn nnff n’n’
yyoo y’y’
H’H’
h’h’x’x’
f’f’
’’
h’ = - ( f’ - x’ )h’ = - ( f’ - x’ )
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Cardinal points of a thick lens
0'
' oyDCBAy
''
'
0
0
fyCy
Ayy
o
LnPdPPP
nfC 21
21'1
'1
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Cardinal points of a thick lens
oo CyxAy
xy
''
''
CAx '
CAfxfh ')''('
CA
CA
Ch 11'
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Cardinal points of a thick lens
'
1 1
nPC
nPdAL
Pn
ndP
CAh
L
'1' 1
Recall that for a thick lensRecall that for a thick lens
PP
nndhL
1'' As we have found beforeAs we have found before
h can be recovered in a similar h can be recovered in a similar manner, along with other manner, along with other cardinal pointscardinal points
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Aberrations
A mathematical treatment can be developed by expanding the sine and tangent terms used in the paraxial approximation
ChromaticChromatic MonochromaticMonochromatic
Unclear Unclear imageimage
Deformation Deformation of imageof image
SphericalSpherical
ComaComa
astigmatismastigmatism
DistortionDistortion
CurvatureCurvature
n (n (λλ))
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Aberrations: Chromatic
Because the focal length of a lens depends on the refractive index (n), and this in turn depends on the wavelength, n = n(λ), light of different colors emanating from an object will come to a focus at different points.
A white object will therefore not give rise to a white image. It will be distorted and have rainbow edges
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Aberrations: Spherical This effect is related to rays which make large angles relative to the
optical axis of the system Mathematically, can be shown to arise from the fact that a lens has a
spherical surface and not a parabolic one Rays making significantly large angles with respect to the optic axis
are brought to different foci
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Aberrations: Coma An off-axis effect which appears when a bundle of incident rays all make the
same angle with respect to the optical axis (source at ∞) Rays are brought to a focus at different points on the focal plane Found in lenses with large spherical aberrations An off-axis object produces a comet-shaped image
ff
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Aberrations: Astigmatism and curvature of field
Yields elliptically distorted imagesYields elliptically distorted images
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Aberrations: Pincushion and Barrel Distortion
This effect results from the difference in lateral magnification of the lens.
If f differs for different parts of the lens,
o
i
o
iT y
yssM will differ alsowill differ also
objectobject Pincushion imagePincushion image Barrel imageBarrel image
ffii>0>0 ffii<0<0
M on axis less than off M on axis less than off axis (positive lens)axis (positive lens)
M on axis greater than M on axis greater than off axis (negative lens)off axis (negative lens)
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Stops in Optical SystemsIn any optical system, one is concerned with a number of things
including:
1. The brightness of the image
S S’
Two lenses of the same Two lenses of the same focal length (focal length (f)f), but , but diameter (D) differsdiameter (D) differs
More light collected More light collected from S by larger from S by larger lenslens
Bundle of Bundle of rays from S, rays from S, imaged at S’ imaged at S’ is larger for is larger for larger lenslarger lens
Image of S Image of S formed at formed at the same the same place by place by both lensesboth lenses
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Stops in Optical Systems Brightness of the image is determined primarily by
the size of the bundle of rays collected by the system (from each object point)
Stops can be used to reduce aberrations
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Stops in Optical SystemsHow much of the object we see is determined by:How much of the object we see is determined by:
(b) The field of View(b) The field of View
Q’Q’(not seen)(not seen)
Rays from Q do not pass through systemRays from Q do not pass through system
We can only see object points closer to the axis of the systemWe can only see object points closer to the axis of the system
Field of view is limited by the systemField of view is limited by the system
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Theory of Stops
We wish to develop an understanding of how and where the bundle of rays are limited by a given optical system
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Aperture Stop
A stop is an opening (despite its name) in a series of lenses, mirrors, diaphragms, etc.
The stop itself is the boundary of the lens or diaphragm
Aperture stop: that element of the optical system that limits the cone of light from any particular object point on the axis of the system
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Aperture Stop: Example
OO
AS