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Lateral resolution (∆x)
Ability to resolve structure across the retina
Limited by PSF size or airy disk size
Pupil size → Diffraction + Aberrations

Axial resolution (∆z)
Resolve structure along the Z-axis (In and out) of the retina
Depth
Limited by the imaging method used

What size lateral and axial resolution is best?
Low (∆z) and low (∆x)
How to determine lateral resolution in diffraction-limited system
Rayleigh criterion
f → Focal length (mm)
D → Aperture diameter

Rayleigh criterion states…
Two point sources can be identified if they are separated by the radius of their airy disks

For 550 nm light, what is the optimal pupil diameter for rayleigh criterion?
Assume: 22mm focal length
∆x = 1.22 * f * λ / D AND Foveal cones are 2.5 microns
The optimal pupil size is 6mm (Image)
Without aberrations

Imaging cones
Refers to individual foveal cones being used as a benchmark for imaging
Foveal cone size = 2.5 microns or 0.5 arc mins
Requirements
6mm pupil
Diffraction-limited system (Rayleigh criterion)
Requirements to resolve one “cycle”
One black-white pair needs to fall on two adjacent cones
∆x of…
5 microns
1 min arc
60 CPD
Is it easier imaging cones in the periphery or fovea?
Peripheral cones!
Why?
They get bigger as you move away from the fovea
Time to reclass bro
Absorption of macular pigment
400nm to 550nm light
Peak near 458nm
Absorption of melanin in the RPE and choroid
Absorption ↓ as wavelength ↑
Absorption patterns of retinal vasculature
Blood absorbs between 400 and 450nm light
Light between 520nm and 590nm is dependent on oxygenation of hemoglobin
Is foveal or parafoveal reflectance greater?
Parafoveal reflectance
Foveal cones have more short wavelength-absorbing pigment
What wavelengths are used for retinal imaging? Why?
700 to 900 nm (Near infrared)
Not absorbed by retinal structures
Less visible to subject → Less photophobia
Things that will fuck up retinal imaging
Accommodation
Tear film between blinks
Fixational eye movements
Patient becomes uncomfortable → Moves around
Adaptive optics (AO) systems
Compensates for fluctuations in accommodation and tear film changes during retinal imaging
Continuously monitors quality of retinal image
Adjusts according to changes in accommodation/tear film
Fixational eye movements
Factor degrading retinal imaging quality
Displace image up to 10 microns
Solution
Short imaging exposure
<10 msec
Eye tracking recordings
Confocal scanning laser ophthalmoscope (cSLO)
Problem: Each retinal layer scatters light differently → Image quality degraded
cSLO solution
Excludes scattered light from every layer except the one of interest
Via a pin-hole that only allows reflected light from the desired layer

cSLO is used in the diagnosis of…
Glaucoma
Macular degeneration
Retinal disorders
How exactly does a cSLO work?
Horizontal and vertical scanning mirrors move laser over the retina (Raster scan)
Uses reflected intensity from each spot to form the image
Pinhole used to only focus the reflected light from the plane you want to image at (Image)
Confocal = The desired layer is in line with the pinhole

Optical sectioning
Changing the layer of the retina that us confocal with the cSLO pinhole allows high resolution image of different sections of the optical media
Can form a 3D scan based on individual images
Axial resolution of cSLO is dependent on…
Dependent on f-number
focal length / D

What is numerical aperture?
Math concept relating f-number to cSLO imaging
NA = 1 / (2 * f #)

Equation to determine axial resolution (∆z) of cSLO

Factors lowering axial resolution
𝛥z= 1.4𝛌/NA2
𝛥z= 5.6𝛌 f/#2
f/# = f / D
Smaller pupil
↓ D = ↑ f/# = ↑ ∆z = Lower resolution
Longer wavelength
Uncorrected aberrations
Optical coherence tomography (OCT) offers very high…
Axial resolution (∆z)
OCT is analogous to what type of imaging?
Ultrasound
Ultrasound
Measures time for sound to bounce back
Axial resolution ~100um
OCT
Measures time for light to bounce back
Axial resolution ~5-10um
Two main types of OCT’s
Time domain OCT
Spectral (Fourier) domain OCT
Low-coherence interferometry
Refers to interferometer emitting a beam but…
Light source is only “coherent” over a short distance before dissociating

How do OCT’s induce short coherence lengths?
Light source of super-luminescent diode (SLD)
How does an OCT work?
OCT shoots short coherence light onto the retina
One beam is reflected from the tissue sample
One beam reflected off mirror in the OCT
Both beams interfere with each other over a short distance
Limitation in distance allows you to pinpoint the depth at which the interference signal is coming from
Therefore axial resolution of the OCT = coherence length of the source
Time-domain OCT (TD-OCT)
Measures interference as a function of tissue depth
Reference and tissue beam shoot out (Normal OCT)
Mirror inside OCT moves around measuring
Depth of signal
Intensity of reflected ‘echoes’
Generates an A-scan
Spectral (Fourier) OCT
Stationary reference mirror (Contrast to TD-OCT)
Spectrometer separates reflected light by wavelength
Resulting interpretation measures depth of scan to form OCT image
Faster than TD-OCT
A,B,C scans
A scan → Single axial scan
B scan → Series of A scans across the retina, retinal slice
C scan → Vertical stack of B-scans in coronal plane
Equation for axial resolution of OCTs

Bandwidth
Refers to the range of wavelengths within a light source
Lasers → Narrow bandwidth
SLDs → Broader bandwidth
Best combined SD-OCT and cSLO system
Heidelberg engineering cSLO and OCT
Adaptive optics systems can be applied to…
Fundus cameras
SLO
OCT
3 main components of adaptive optics systems
Wavefront sensor (WFS)
Measures wavefront aberrations
Wavefront corrector
Corrects aberrations with deformable mirror
Control computer
Controls the WFS and DM