mit 2.71/2.710 optics 11/08/04 wk10-a- 1 today imaging with coherent light coherent image formation...
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![Page 1: MIT 2.71/2.710 Optics 11/08/04 wk10-a- 1 Today Imaging with coherent light Coherent image formation –space domain description: impulse response –spatial](https://reader033.vdocuments.us/reader033/viewer/2022051819/55150200550346a80c8b5445/html5/thumbnails/1.jpg)
MIT 2.71/2.710 Optics 11/08/04 wk10-a-1
Today
Imaging with coherent light
• Coherent image formation
–space domain description: impulse response
–spatial frequency domain description: coherent transfer function
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-2
The 4F system
Fourier transform
relationship
Fourier transform
relationship
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-3
The 4F system
Theorem:
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-4
The 4F system
object plane
Fourier plane Image plane
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-5
The 4F system
object plane
Fourier plane Image plane
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-6
The 4F system with FP aperture
object plane Fourier plane : aperture-limitedImage plane: blurred i. e. low-pass filtered
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-7
Impulse response & transfer function
A point source at the
input plane ...
... results not in a point image but in a diffraction pattern h(x’,
y’)
Point source at the origin ↔delta function δ(x,y) h(x’,y’) is the inpulse response of the system
More commonly, h(x’,y’) is called the
Coherent Point Spread Function (Coherent PSF)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-8
Coherent imaging as a linear, shift-invariant system
transfer function H(u,v): akapupil function
Thin transparencyoutput
amplitude
impulse response
convolution
Fourier transform
Fourier transform
illumi nation
(≡plane wave spectrum
transfer function
multiplication
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-9
Transfer function & impulse responseof rectangular aperture
Transfer function:circular aperture
Impulse response:Airy function
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-10
Coherent imaging as a linear, shift-invariant system
Example: 4F system with circular aperture @ Fourier plane
Thin transparency
illumination
Impulse response
output amplitude
Fouriertransform
Fouriertransform
transfer function
multiplication
convolution
(≡plane wave spectrum
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-11
Transfer function & impulse responseof rectangular aperture
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-12
Coherent imaging as a linear, shift-invariant system
Example: 4F system with circular aperture @ Fourier plane
Thin transparency
illumination
Impulse response
output amplitude
Fouriertransform
Fouriertransform
transfer function
multiplication
convolution
(≡plane wave spectrum
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-13
Aperture–limited spatial filtering
object plane:grating generates
one spatial frequency
Fourier plane:aperture unlimited
Image plane:grating is imaged
with lateralde-magnification
(all orders pass)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-14
Aperture–limited spatial filtering
object plane:grating generates
one spatial frequency
Fourier plane:aperture limited
Image plane:grating is not imaged
only 0th order(DC component)
surviving(some orders cut off)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-15
Spatial frequency clipping
field after input transparency
field before filter
field after filter
field at output(image plane)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-16
Effect of spatial filtering
Fourier plane filterwith circ-aperture
Original object(sinusoidal spatial
variation, i.e. grating)
Frequency-filtered image(spatial variation blurred out,
only average survives)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-17
Spatial frequency clipping f1=20cmλ=0.5μm
monochromatic coherent on-axis
illumination
object planeTransparencyintensity at input plane Intensity before Fourier Filter (negative contrast)
Fourier planecire-aperture
Fourier filter transitivity
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-18
Space-Fourier coordinate transformations
:pixel size :frequencyresolution
sparedomain
SpatialFrequencydomainNyquist
relationships.
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-19
4F coordinate transformations
:pixel size
Nyquistrelationships.
sparedomain
Fourierplane
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-20
Spatial frequency clipping f1=20cmλ=0.5μm
monochromatic coherent on-axis
illumination
object planetransparencyintensity at input plane Intensity before Fourier Filter (negative contrast)
Fourier planecire-aperture
Fourier filter transitivity
Image planeobserved field
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-21
Formation of the impulse response
object plane:pinhole generates
spherical waveFourier plane:
circ-aperture limited
Image plane:Fourier transform
of aperture,Airy pattern
(plane wave is clipped)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-22
field after input transparency
field before filter
field after filter
field at output(image plane)
Low–pass filtering
(Airy pattern)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-23
Effect of spatial filtering
Fourier plane filterwith circ-aperture
Original object(small pinhole ⇔impulse, generating spherical wave
past the transparency)
Impulse reponse (aka point point-spread function,
original point has blurred to an Airy pattern, or jinc)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-24
Low–pass filtering the impulse f1=20cmλ=0.5μm
monochromatic coherent on-axis
illumination
object planetransparency
intensity at input plane Intensity before Fourier Filter (negative contrast)
Fourier planecire-aperture
Fourier filter transitivity
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-25
Spatial frequency clipping
monochromatic coherent on-axis
illumination
object planetransparency
intensity at input plane Intensity after Fourier filter
Fourier planecire-aperture
Intensity at output plane
Image planeobserved field
note: pseudo-accentuated sidelobes
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-26
Low-pass filtering with the 4F system
monochromatic coherent on-axis
illumination
object planetransparency
Fourier planecire-aperture
Image planeobserved field
field arrivingAt Fourier plane
field arrivingfrom Fourier plane
Fouriertransform
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-27
monochromatic coherent on-axis
illumination
object planetransparency
Fourier planecire-aperture
Image planeobserved field
Spatial filtering with the 4F system
field arrivingAt Fourier plane
field arrivingfrom Fourier plane
Fouriertransform
Fouriertransform
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-28
Examples: the amplitude MIT pattern Original MIT pattern
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-29
Weak low–pass filtering
Pinhole, radius 2.5mm Filtered with pinhole, radius 2.5mm
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-30
Moderate low–pass filtering(aka blurringblurring)
Fourier filter Intensity @ image plane
Pinhole, radius 1mm Filtered with pinhole, radius 1mm
f1=20cmλ=0.5μm
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-31
Strong low–pass filtering
Pinhole, radius 0.5mm Filtered with pinhole, radius 0.5mm
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-32
Moderate high–pass filtering
Reflective disk, radius 0.5mm Filtered with reflective disk, radius 0.5mm
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-33
Strong high–pass filtering
Reflective disk, radius 2.5mm Filtered with reflective disk, radius 2.5mm
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
(aka edge enhancement)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-34
1-dimensional blurring
Horizontal slit, width 2mm Filtered with horizontal slit, width 2mm
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-35
1-dimensional blurring
vertical slit, width 2mm Filtered with vertical slit, width 2mm
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-36
Phase objects
glass plate(transparent)
thickness
protruding partphase-shifts
coherent illuminationby amount φ=2π(n-1)t/λ
Often useful in imaging biological objects (cells, etc.)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-37
Viewing phase objects
Intensity(object is invisible)
Amplitude(need
interferometer)
Original phase MIT pattern (intensity) Original 0.1 rad phase MIT pattern (phase)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-38
Zernicke phase-shift mask
phase-shift mask (magnitude), radii 5mm & 1mm phase-shift mask (phase), radii 5mm & 1mm (phase)
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-39
Imaging with Zernicke mask
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
phase-shift mask (phase), radii 5mm & 1mm (phase) phase-shift mask, radii 5mm & 1mmFiltered with,
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MIT 2.71/2.710 Optics 11/08/04 wk10-a-40
Imaging with Zernicke mask
Fourier filter Intensity @ image plane f1=20cmλ=0.5μm
phase-shift mask (phase), radii 5mm & 0.1mm (phase) phase-shift mask, radii 5mm & 0.1mmFiltered with,