review of basic principles in optics, wavefront and
TRANSCRIPT
Review of Basic Principles in Optics, Wavefront and Wavefront Error
Austin Roorda, Ph.D.University of California, Berkeley
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Geometrical Optics
Relationships between pupil size, refractive error and
blur
Optics of the eye: Depth of Focus
2 mm 4 mm 6 mm
2 mm 4 mm 6 mm
Optics of the eye: Depth of Focus
Focused behind retina
In focus
Focused in front of retina
DemonstrationRole of Pupil Size and Defocus on Retinal Blur
Draw a cross like this one on a page. Hold it so close that is it completely out of focus, then squint. You should see the horizontal line become clear. The line becomes clear because you have used your eyelids to make your effective pupil size smaller, thereby reducing the blur due to defocus on the retina image. Only the horizontal line appears clear because you have only reduced the blur in the horizontal direction.
Computation of Geometrical Blur Size
blur[mrad] [ ]blur[minutes] 3.44 [ ]
D pupilsize mmD pupilsize mm
= ×= × ×
where D is the defocus in diopters
Application of Blur Equation
• 1 D defocus, 8 mm pupil produces 27.52 minute blur size ~ 0.5 degrees
Physical Optics
The Wavefront
What is the Wavefront?parallel beam
=plane wavefront
converging beam=
spherical wavefront
What is the Wavefront?parallel beam
=plane wavefront
ideal wavefront
defocused wavefront
What is the Wavefront?parallel beam
=plane wavefront
ideal wavefront
aberrated beam=
irregular wavefront
What is the Wavefront?diverging beam
=spherical wavefront
aberrated beam=
irregular wavefront
ideal wavefront
The Wave Aberration
What is the Wave Aberration?diverging beam
=spherical wavefront wave aberration
-3 -2 -1 0 1 2 3
-3
-2
-1
0
1
2
3
Wavefront Aberration
mm (right-left)
mm
(sup
erio
r-inf
erio
r)
Wave Aberration: Defocus
Wave Aberration: Coma
-3 -2 -1 0 1 2 3
-3
-2
-1
0
1
2
3
Wavefront Aberration
mm (right-left)
mm
(sup
erio
r-inf
erio
r)
Wave Aberration: All Terms
-3 -2 -1 0 1 2 3
-3
-2
-1
0
1
2
3
Wavefront Aberration
mm (right-left)m
m (s
uper
ior-i
nfer
ior)
Zernike Polynomials
Wave Aberration Contour Map
0-2.5
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
mm (right-left)
mm
(sup
erio
r-inf
erio
r)
-2 -1 1 2
Breakdown of Zernike TermsCoefficient value (microns)-0.5 0 0.5 1 1.5 2
123456789
1011121314151617181920
Zern
ike
term
astig.defocus
astig.trefoilcomacomatrefoil
spherical aberration
2nd order
3rd order
4th order
5th order
The Reason we Measure the Wave Aberration
PTF (phase)
PSF(point spread function)
OTF (optical transfer function)
MTF (contrast)
Image Quality Metrics
The Point Spread Function
The Point Spread Function, or PSF, is the image that an optical system forms of a point
source.
The point source is the most fundamental object, and forms the basis for any complex
object.
The PSF is analogous to the Impulse Response Function in electronics.
The Point Spread Function
The PSF for a perfect optical system is the Airy disc, which is the Fraunhofer diffraction
pattern for a circular pupil.
Airy Disc
Airy Disk
θ
1.22aλθ ⋅
=
angle subtended at the nodal point
wavelength of the light
pupil diametera
θ
λ
≡
≡
≡
As the pupil size gets larger, the Airy disc gets smaller.
angle subtended at the nodal point
wavelength of the light
pupil diameter
1.22
a
aθ
λ
λθ
≡
≡
≡
⋅=
0
0.5
1
1.5
2
2.5
1 2 3 4 5 6 7 8
pupil diameter (mm)
PS
F A
iry D
isk
radi
us (m
inut
es)
Point Spread Function vs. Pupil Size
1 mm 2 mm 3 mm 4 mm 5 mm 6 mm 7 mm
Perfect Eye
Typical Eye
Resolution
Rayleighresolution
limit
Unresolved point sources
Resolved
As the pupil size gets larger, the Airy disc gets smaller.
min
min
angle subtended at the nodal point
wavelength of the light
pupil diameter
1.22
a
aθ
λ
λθ
≡
≡
≡
⋅=
0
0.5
1
1.5
2
2.5
1 2 3 4 5 6 7 8
pupil diameter (mm)
PS
F A
iry D
isk
radi
us (m
inut
es)
Keck telescope: (10 m reflector) About 4500 times better than the eye!
Convolution
Convolution
( , ) ( , ) ( , )PSF x y O x y I x y⊗ =
Simulated Images
20/40 letters
20/20 letters
MTFModulation Transfer
Function
low medium high
object:100% contrast
image
cont
rast
1
0spatial frequency
MTF: Cutoff Frequency
0
0.5
0
2 mm4 mm6 mm8 mm
mod
ulat
ion
tran
sfer
cut-off frequency
57.3cutoffafλ
=⋅
Rule of thumb: cutoff frequency increases by ~30 c/d for each mm increase in pupil size
1 mm1
50 100 150 200 250 300spatial frequency (c/deg)
Modulation Transfer Function
vertical spatial frequency (c/d) horizontal spatial
frequency (c/d)
0.2
0.4
0.6
0.8
-100 0 100c/deg
PTFPhase Transfer
Function
low medium high
object
image
phas
e sh
ift
0
-180
180
spatial frequency
Phase Transfer Function
• Contains information about asymmetry in the PSF
• Contains information about contrast reversals (spurious resolution)
The Importance of Phase
Relationships Between Wave Aberration,
PSF and MTF
The Reason we Measure the Wave Aberration
PTF (phase)
PSF(point spread function)
OTF (optical transfer function)
MTF (contrast)
Image Quality Metrics
The PSF is the Fourier Transform (FT) of the pupil function
( )2 ( , )
, ( , )i W x y
i iPSF x y FT P x y eπλ
− =
The MTF is the amplitude component of the FT of the PSF
( ) { }, ( , )x y i iMTF f f Amplitude FT PSF x y=
The PTF is the phase component of the FT of the PSF
( ) { }, ( , )x y i iPTF f f Phase FT PSF x y=
The OTF (MTF and PTF) can also be computed as the autocorrelation of the pupil function
Point Spread FunctionWavefront Aberration
-0.5
0
0.5
-200 -100 0 100 200-2 -1 0 1 2arcsecmm (right-left)
c/deg-100 0 100
0.2
0.4
0.6
0.8
c/deg-100 0 100
-0.5
0
0.5
Modulation Transfer Function Phase Transfer Function
Point Spread FunctionWavefront Aberration
-0.5
0
0.5
-2 -1 0 1 2 -200 -100 0 100 200mm (right-left) arcsec
Modulation Transfer Function Phase Transfer Function
0.2
0.4
0.6
0.8
-150
-100
-50
0
50
100
150
-100 0 100 -100 0 100c/deg c/deg
Point Spread FunctionWavefront Aberration
-0.5
0
0.5
1
1.5
-2 -1 0 1 2 -1000 -500 0 500 1000mm (right-left) arcsec
Modulation Transfer Function Phase Transfer Function
0.2
0.4
0.6
0.8
-150
-100
-50
0
50
100
150
-100 0 100 -100 0 100c/deg c/deg
Conventional Metrics to Define Imagine Quality
Root Mean Square
( ) ( )( )
( )( )
21 , ,
pupil area, wave aberration
, average wave aberration
RMS W x y W x y dxdyA
AW x y
W x y
= −
−
−
−
∫∫
Root Mean Square: Advantage of Using Zernikes to
Represent the Wavefront
( ) ( ) ( ) ( )2 2 2 22 0 2 12 2 2 3 .......RMS Z Z Z Z− −= + + +
astig
matism
term
defoc
us te
rm
term
trefoi
l term ……
astig
matism
Strehl Ratio
diffraction-limited PSF
Strehl Ratio = eye
dl
HHHdl
actual PSF
Heye
Modulation Transfer Function
0.30.40.50.6
cont
rast Area under the MTF
20/20 20/10
10.90.80.7
0.20.1
00 50 100 150
spatial frequency (c/deg)
Metrics to Define Image Quality
Other Metrics
Campbell,C.E. (2004). Improving visual function diagnostic metrics with the use of higher-order aberration information from the eye. J.Refract.Surg. 20, S495-S503
Cheng,X., Bradley,A., Hong,X., & Thibos,L. (2003). Relationship between refractive error and monochromatic aberrations of the eye. Optom.Vis.Sci. 80, 43-49.
Cheng,X., Bradley,A., & Thibos,L.N. (2004). Predicting subjective judgment of best focus with objective image quality metrics. J.Vis. 4, 310-321.
Guirao,A. & Williams,D.R. (2003). A method to predict refractive errors from wave aberration data. Optom.Vis.Sci. 80, 36-42.
Marsack,J.D., Thibos,L.N., & Applegate,R.A. (2003). Scalar metrics of optical quality derived from wave aberrations predict visual performanc. J.Vis. 4, 322-328.
Sarver,E.J. & Applegate,R.A. (2004). The importance of the phase transfer function to visual function and visual quality metrics. J.Refract.Surg. 20, S504-S507
Typical Values for Wave Aberration
Strehl Ratio
• Strehl ratios are about 5% for a 5 mm pupil that has been corrected for defocus and astigmatism.
• Strehl ratios for small (~ 1 mm) pupils approach 1, but the image quality is poor due to diffraction.
Typical Values for Wave AberrationPopulation Statistics
spherical aberration
comacomatrefoil
trefoil
Typical Values for Wave AberrationChange in aberrations with pupil size
rms
wav
e ab
erra
tion
(mic
rons
) Shack Hartmann MethodsOther Methods
1.2Iglesias et al, 1998Navarro et al, 1998Liang et al, 1994Liang and Williams, 1997Liang et al, 1997Walsh et al, 1984He et al, 1999Calver et al, 1999Calver et al, 1999Porter et al., 2001He et al, 2002He et al, 2002Xu et al, 2003Paquin et al, 2002Paquin et al, 2002Carkeet et al, 2002Cheng et al, 2004
1
0.8
0.6
0.4
0.2
00 1 2 3 4 5 6 7 8 9
pupil size (mm)
Typical Values for Wave AberrationChange in aberrations with age
Monochromatic Aberrations as a Function of Age, from Childhood to Advanced AgeIsabelle Brunette,1 Juan M. Bueno,2 Mireille Parent,1,3 Habib Hamam,3 and Pierre Simonet3
Other Optical Factors that Degrade Image Quality
Retinal Sampling
Sampling by Foveal Cones
Projected Image Sampled Image
5 arc minutes20/20 letter
Sampling by Foveal Cones
5 arc minutes20/5 letter
Projected Image Sampled Image
Nyquist Sampling Theorem
Photoreceptor Sampling >> Spatial Frequency1
I
0
I
0
1
nearly 100% transmitted
Photoreceptor Sampling = 2 x Spatial Frequency1
I
0
I
0
1
nearly 100% transmitted
Photoreceptor Sampling = Spatial Frequency1
I
0
I
0
1
nothing transmitted
Nyquist theorem:The maximum spatial frequency that can be detected is equal to ½ of the sampling frequency.
foveal cone spacing ~ 120 samples/deg
maximum spatial frequency: 60 cycles/deg (20/10 or 6/3 acuity)
MTF: Cutoff Frequency
0
0.5
0
1 mm2 mm4 mm6 mm8 mm
mod
ulat
ion
tran
sfer
cut-off frequency
57.3cutoffafλ
=⋅
Rule of thumb: cutoff frequency increases by ~30 c/d for each mm increase in pupil size
Nyquist limit
1
50 100 150 200 250 300spatial frequency (c/deg)
Thankyou!