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Optical Aberrations Resident Lecture
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Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Dec 31, 2015

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Page 1: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Optical Aberrations

Resident Lecture

Page 2: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

The Perfect Image

There is no such thing as a perfect image

                           

                  

All light rays passing through optical systems are subject to distortions

Page 3: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Outline

Chromatic Aberration Spherical Aberration Oblique Astigmatism Coma Curvature of Field Distortion

Point Spread Function

Modulation Transfer Wavefront Analysis Custom Lasik and

Zernicke Polynomials

Page 4: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Chromatic Aberration

A lens will not focus different colors in exactly the same place.

the focal length depends on refraction and the index of refraction

Short wavelength has higher n and is refracted more than long wavelength

The amount of chromatic aberration depends on the dispersion of the glass.

Lens

Eye

http://micro.magnet.fsu.edu/primer/java/aberrations/spherical/index.html

Page 5: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Chromatic Aberration

Dispersive power (abbe value) is based on change in index for different wavelengths

If the index is the same for all wavelengths, there is NO DISPERSION

The n increases as wavelength decreases

Page 6: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Chromatic Aberration

Some patients can detect this Dispersion usually increases in high index May be noticeable with IOL’s

Page 7: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Chromatic AberrationDuochrome Test

Duochrome test helps you determine position of focal point with respect to the fovea

Useful to avoid overminusing pt.

  

Page 8: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Duochrome Test

Too much minus greenis clearer

Too much plus red is clearer

Page 9: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Chromatic Aberration-Duochrome Test

Red clarity= green claritythen image is positionedcorrectly.

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Page 10: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Correction of Chromatic Aberration

An achromat doublet does not completely eliminate chromatic aberration, but can eliminate it for two colors, say red and blue.

The idea is to use a lens pair – a strong lens of low dispersion coupled with a weaker one of high dispersion calculated to match the focal lengths for two chosen wavelengths.

Cemented doublets of this type are a mainstay of lens design.

Achromatic Doublets

Page 11: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Correction of Chromatic Aberration

APOCHROMATIC LENS The addition of a third lens corrects for three colors (red, blue and green), greatly reducing the fuzziness caused by the colors uncorrected in the achromatic doublet.

Page 12: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Correction of Chromatic Aberration

In the human eye, chromatic aberration is reduced by the lens, which changes index from the nucleus outward.

Page 13: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Spherical Aberration

For lenses made with spherical surfaces, rays which are parallel to the optic axis but at different distances from the optic axis fail to converge to the same point.

                                                                                                                            

        

http://www.olympusmicro.com/primer/java/aberrations/spherical

Page 14: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Spherical Aberration- correction

Spherical aberration in the human eye is reduced by the aspheric shape of the lens and the cornea

Page 15: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Spherical Aberration- Correction

Meniscus LensesThe amount of spherical aberration in a lens made from spherical surfaces depends upon its shape. Best form, depends on base curve       

Page 16: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Oblique Astigmatism

This aberration primarily influences the image quality of spherical lenses. When the wearer looks at an angle through the lens, there is a deviation which he perceives as blur. The higher the dioptric power of the lens, the more pronounced this error becomes.

Page 17: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Oblique Astigmatism

                              

                              

                              

                              

A dot is no longer imaged as a dot, but as two image lines.

Page 18: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Oblique astigmatism- correction

Mitigated by deviating from the spherical shape

Aspheric Surfaces to the Rescue

   

Page 19: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Coma

. Coma is an aberration which causes rays from an off-axis point of light in the object plane to create a trailing "comet-like" blur directed away from the optic axis.

Page 20: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Coma

A lens with

considerable coma may produce a sharp image in the center of the field, but become increasingly blurred toward the edges.

Page 21: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Coma

      The resulting image is called a comatic circle. The coma flare, which owes its name to its cometlike tail, is often considered the worst of all aberrations, primarily because of its asymmetric configuration.

Page 22: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Coma- correction

For a single lens, coma can be partially corrected by bending the lens. More complete correction can be achieved by using a combination of lenses symmetric about a central stop.

Coma is not well compensated for in the human eye.

Page 23: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Curvature of Field

Causes an planar object to project a curved (nonplanar) image. It can be thought of as arising from a "power error" for rays at a large angle. Those rays treat the lens as having an effectively smaller diameter and an effectively higher power, forming the image of the off axis points closer to the lens.

Page 24: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Curvature of Field

A lens aberration that causes a flat object surface to be imaged onto a curved surface rather than a plane.  

http://www.microscopyu.com/tutorials/java/aberrations/curvatureoffield/

=n*f2

Page 25: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Curvature of Field- Correction

The surface of the image formed by the eye is also curved, fortunately, the retina is also curved!

For lens systems, using best form lenses with non-spherical shapes can help.

Page 26: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Image Distortion

Not about sharpness, but faithful reproduction of the shape of the object.

It occurs when magnification varies with the distance of the object from the optic axis.

Problem only for high powers Tends to falsify the positions of objects and

cause vertical lines to wave Aphakes! Minimized by very steep back base curves

Page 27: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Image Distortion

Plus lens Minus lens

Page 28: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Outline

Chromatic Aberration Spherical Aberration Oblique Astigmatism Coma Curvature of Field Distortion

Point Spread Function

Modulation Transfer Wavefront Analysis Custom Lasik and

Zernicke Polynomials

Page 29: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Beyond sphere and cylinder…

Higher order aberrations have been traditionally ignored clinically

Now are routinely considered Post lasik increase in higher order aberrations Can be easily measured Wavefront guided correction available Patient expectations

Page 30: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

History of wavefront sensing

DOD in the 1980’s to support “star wars” Measure the constantly fluctuating refractive power of the

atmosphere to improve accuracy of satellite photos and accuracy of weapons

Led to adaptive optics – real time measurements of refractions using “deformable mirrors” that rapidly

Astronomers were interested to improve telescope images

www.opt.pacificu.edu

Page 31: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Shack-Hartmann wavefront sensor

Hartmann first looked at this a century agoShack elaborated on this in the 1980’s

working for the air forceLiang was the first to use the wavefront

sensor to measure the human eye in 1994.

By the late 1990’s commercial development was occuring.

Page 32: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Airy Disc

When wave encounters and obstruction, the direction of the wave changes.

This is called DIFFRACTION

An Airy disc shows how a point image is degraded by aberration

Page 33: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.
Page 34: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Point Spread Function

Consider an object consisting of a perfect point. The image of this object will be at least one point wide. Normally it’s image will consist instead of a spot of several points, brightest in the centre and progressively darker away from the centre. This image function is the point-spread function.

Page 35: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Point Spread Function

used to assess the spatial resolution of an imaging system.

The PSF need not be symmetrical, so there may be different spatial resolutions in different directions.

Note that the PSF is, in most cases, a function with significant variation over the field of view.

Page 36: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Modulation Transfer Function

Used to assess the overall spatial resolution of an imaging system. It is formally defined as the magnitude of the Fourier transformed point spread function

The concept of the MTF is to portray how much of the contrast at a specific resolution is maintained by the imaging process.

Page 37: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Modulation Transfer Function

How can the degradation of an optical system be evaluated?

SQUARE WAVE

Max luminance

Min luminance

Modulation= Lmax-Lmin/Lmax+Lmin

Page 38: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Modulation Transfer Function

Square wave grating of specific frequency and contrast is passed through an optical system. The MODULATION can then be measured

MTF= Mi/Mo Luminance of stimulus

Luminance of image

Page 39: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Modulation Transfer Function

In the optimal case, the MTF value is 1 meaning that object and image contrast are identical.

MTF usually starts with a value 1 at 0 spatial frequency which represents a homogeneous background. It then drops in a system-specific manner down to zero. By using the MTF, two systems can readily be compared: At each spatial frequency (or 1/resolution) that system with the higher MTF maintains better contrast.

Page 40: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront analysis (wavescan)

Light is has both particle and wave characteristics

Wavefront analysis describes the wave behavior of light in the eye

Actual image displacement of the point source from foveola as it passes through the optical system of the eye compared to the ideal image.

Page 41: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Custom Lasik-Wavescan

Wavescan uses the principles of MTFCustom can correct for

Myopia or hyperopia Astigmatism Spherical Aberration Coma

Custom does not correct for Chromatic aberration Diffraction

Page 42: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Hartmann-Shack AberrommetryHow does it work….

Analyze light that emerges or is reflected from the retina and passes through the optical system of the eye.

Produces a “fingerprint” of the aberrations for an individual eye.

Page 43: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Measuring Aberrations

Emmetropia/ no aberrations

Myopia/distorted wavefront

Aberrometers measure the shape of the wavefront

Page 44: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront analysis

The distance between the wavefront surface and a reference plane

Wavefront exitingThe eye. Distance From the referencePlane is measured At many points.

Page 45: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Hartmann Shack aberrometer

Each lenslet is a fraction of a mm. It divides the broad beam of lightInto many sub-beams for measurement. Each lenslet focuses onto the Video sensor. We analyze the position of each spot.

Page 46: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront Analysis

Page 47: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront Analysis

In an aberration free eye dot is centered and focused with respectTo a grid/array.

Page 48: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront Analysis

Page 49: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront Analysis

Sometimes it is easier to visualize the wavefront in a 3D surface plot

Page 50: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront Analysis

Spherical Aberration

Astigmatism

Trefoil

Quadrafoil

Page 51: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront Analysis – Root Mean Square

Measure of the deviation of an actual image from an ideal image of the source point object

RMS of ideal system is 0RMS of human eye increases from 0.1 to

0.25 at 60yo.Standard LASIK increases RMS especially

for large pupils.

Page 52: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

What are Zernicke polynomials?

Monochromatic aberrations can be decomposed into Zernicke polynomials

Each ZP corresponds to a specific geometric pattern of aberration and are grouped into orders

These are mathematical expressions that describe how much of what type of geometric pattern is contributing to the total wavefront aberration.

Basically it is a system for categorizing higher order aberrations

Page 53: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront Errors describedBy Zernicke analysis

Page 54: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Custom Lasik- Zernicke Polynomials

Each mode will have a number that is + or -. This coefficient tells you how much of that aberration is present

The units are not diopters, but microns Pupil size is included Will give you RMS Zernicke modes are grouped into orders

2nd order non wavefront 3rd order and above are “higher order”. They are labelled

using a double index scheme Znm, where n refers to the

order and m to the mode within the order. Some of the modes have names

Page 55: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Higher order aberrations and relative risk of symptoms after LASIK. Sharma M, Wachler BS, Chan CC.

RESULTS: Blurring of vision was the most common symptom (41.6%) followed by double image (19.4%), halo (16.7%), and

fluctuation in vision (13.9%) in symptomatic patients. A statistically significant difference was noted in UCVA (P

= .001), BSCVA (P = .001), contrast sensitivity (P < .001), and manifest cylinder (P = .001) in the two groups. The percentage difference between the symptomatic and control group mean root-mean-square (RMS) values ranged from 157% to 206% or 1.57 to 2.06 times greater. CONCLUSIONS: Patients with visual symptoms after LASIK have significantly lower visual acuity and contrast sensitivity and higher mean RMS values for higher order aberrations than patients without symptoms.

Root-mean-square values of greater than two times the normal after-LASIK J refractive surgery March 2007

Ocular higher-order aberrations and contrast sensitivity after conventional laser in situ keratomileusis Yamane N, Miyata K, Samejima T, IOVS 2004

Page 56: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Summary

Understand that ametropia is not the only thing that causes blurry vision

Understand that aberrations also plague lens systems in glasses, microscopes, etc.

Introduction to how refractive surgery (and IOL’s, spectacls and CLS) is attempting to compensate for aberrations inherent in the optics of the eye.

Page 57: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Presbyopic IOLs

Page 58: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Multifocal IOLs

http://www.eyeclinic.com.br/acrysoft/foto_04.jpg

Page 59: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Apodized diffractive optics for a full range of vision The AcrySof® ReSTOR® IOL was designed to provide a complete range of vision independent of

the ciliary muscle body. To achieve this, the AcrySof® ReSTOR® IOL combines the functions of both apodized diffractive and refractive regions.

Apodized DiffractiveThe apodized diffractive optics are found within the central 3.6 mm optic zone of the lens. This area comprises 12 concentric steps of gradually decreasing (1.3-0.2 microns) step heights that allocate energy based on lighting conditions and activity, creating a full range of quality vision – near to distant.

Refractive

The refractive region of the optic surrounds the apodized diffractive region. This area directs light to a distance focal point for larger pupil diameter, and is dedicated to distance vision.

Apodization for minimal visual disturbances Apodization is the gradual reduction or blending of diffractive step heights. This unique

technology optimally distributes the appropriate amount of light to near and distant focal points, regardless of the lighting situation.

The apodized diffractive optic of the AcrySof® ReSTOR® IOL is designed to improve image quality while minimizing visual disturbances. The result is an increased range of quality vision that delivers a high level of spectacle freedom.

ReStor

Page 60: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

ReZoom

 

Balanced View Optics™ Technology

Page 61: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

ReZoom

Five focusing zones for a full range of vision The ReZoom™ Multifocal Lens has uniquely proportioned visual zones that provide it with its major advantage. Each ReZoom™ Multifocal Lens is divided into five different zones with each zone designed for different light and focal distances.

  

                                                                                                                                                                                                                                          

  

                                                                                                                                                                                                                                          

                                                                                                                                                                                                               

                           

Page 62: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Distance centerNear adjacent Low light near and dist in the peripehryIntermediate one zone

Page 63: Optical Aberrations Resident Lecture. The Perfect Image There is no such thing as a perfect image All light rays passing through optical systems are subject.

Wavefront IOL

Tecnis IOL (AMO)Only wavefront-designed IOL with claims approved by the FDA for reduced spherical aberration, i

The Tecnis Z9001 IOL with a modified prolate anterior surface produces negative spherical aberration and consequently reduces the higher-order aberrations in pseudophakic eyes. This leads to enhanced contrast sensitivity and improved functional vision compared to conventional spherical IOLs.