AST Lab exercise: aberrations

Similar documents
Laboratory experiment aberrations

Lecture 4: Geometrical Optics 2. Optical Systems. Images and Pupils. Rays. Wavefronts. Aberrations. Outline

Waves & Oscillations

Performance Factors. Technical Assistance. Fundamental Optics


Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

Tutorial Zemax Introduction 1

Geometric optics & aberrations

Explanation of Aberration and Wavefront

Chapter 25 Optical Instruments

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember

Astronomy 80 B: Light. Lecture 9: curved mirrors, lenses, aberrations 29 April 2003 Jerry Nelson

Thin Lenses * OpenStax

ECEG105/ECEU646 Optics for Engineers Course Notes Part 4: Apertures, Aberrations Prof. Charles A. DiMarzio Northeastern University Fall 2008

Optical System Design

AST Lab exercise: CCD

Optical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics

IMAGE SENSOR SOLUTIONS. KAC-96-1/5" Lens Kit. KODAK KAC-96-1/5" Lens Kit. for use with the KODAK CMOS Image Sensors. November 2004 Revision 2

Converging and Diverging Surfaces. Lenses. Converging Surface

Optimisation. Lecture 3

Introduction to Optical Modeling. Friedrich-Schiller-University Jena Institute of Applied Physics. Lecturer: Prof. U.D. Zeitner

Lens Design I Seminar 1

Lens Design I. Lecture 5: Advanced handling I Herbert Gross. Summer term

a) How big will that physical image of the cells be your camera sensor?

COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR)

Ch 24. Geometric Optics

UNIVERSITY OF NAIROBI COLLEGE OF EDUCATION AND EXTERNAL STUDIES

Applied Optics. , Physics Department (Room #36-401) , ,

Image Formation. Light from distant things. Geometrical optics. Pinhole camera. Chapter 36

ECEN 4606, UNDERGRADUATE OPTICS LAB

Chapters 1 & 2. Definitions and applications Conceptual basis of photogrammetric processing

Heisenberg) relation applied to space and transverse wavevector

Exercises Advanced Optical Design Part 5 Solutions

Option G 2: Lenses. The diagram below shows the image of a square grid as produced by a lens that does not cause spherical aberration.

Sequential Ray Tracing. Lecture 2

Lecture PowerPoint. Chapter 25 Physics: Principles with Applications, 6 th edition Giancoli

OPTICAL SYSTEMS OBJECTIVES

Lens Design II. Lecture 2: Structural modifications Herbert Gross. Winter term

OPAC 202 Optical Design and Inst.

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name:

25 cm. 60 cm. 50 cm. 40 cm.

Long Wave Infrared Scan Lens Design And Distortion Correction

Lenses. Overview. Terminology. The pinhole camera. Pinhole camera Lenses Principles of operation Limitations

R.B.V.R.R. WOMEN S COLLEGE (AUTONOMOUS) Narayanaguda, Hyderabad.

Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term

PHY170: OPTICS. Things to do in the lab INTRODUCTORY REMARKS OPTICS SIMULATIONS

Cameras, lenses, and sensors

WaveMaster IOL. Fast and Accurate Intraocular Lens Tester

Using Stock Optics. ECE 5616 Curtis

Week IV: FIRST EXPERIMENTS WITH THE ADVANCED OPTICS SET

INTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS

OPAL. SpotOptics. AUTOMATED WAVEFRONT SENSOR Single and double pass O P A L

Introduction. Geometrical Optics. Milton Katz State University of New York. VfeWorld Scientific New Jersey London Sine Singapore Hong Kong

1.1 Singlet. Solution. a) Starting setup: The two radii and the image distance is chosen as variable.

EP118 Optics. Content TOPIC 9 ABERRATIONS. Department of Engineering Physics University of Gaziantep. 1. Introduction. 2. Spherical Aberrations

The Brownie Camera. Lens Design OPTI 517. Prof. Jose Sasian

Lenses Design Basics. Introduction. RONAR-SMITH Laser Optics. Optics for Medical. System. Laser. Semiconductor Spectroscopy.

Flatness of Dichroic Beamsplitters Affects Focus and Image Quality

Announcements. Image Formation: Outline. The course. How Cameras Produce Images. Earliest Surviving Photograph. Image Formation and Cameras

WaveMaster IOL. Fast and accurate intraocular lens tester

Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term

Practical Flatness Tech Note

Aberrations and adaptive optics for biomedical microscopes

Lens Design I. Lecture 10: Optimization II Herbert Gross. Summer term

Design of Large Working Area F-Theta Lens. Gong Chen

Handbook of Optical Systems

Better Imaging with a Schmidt-Czerny-Turner Spectrograph

Exercise 1 - Lens bending

Chapter 18 Optical Elements

GEOMETRICAL OPTICS AND OPTICAL DESIGN

3.0 Alignment Equipment and Diagnostic Tools:

OPTINO. SpotOptics VERSATILE WAVEFRONT SENSOR O P T I N O

OPTICAL IMAGING AND ABERRATIONS

The Basic Scheme of the Afocal System and Composition Variants of the Objectives Based on It

Astro 500 A500/L-8! 1!

Department of Physics & Astronomy Undergraduate Labs. Thin Lenses

Lens Design I Seminar 5

Chapter 36. Image Formation

Big League Cryogenics and Vacuum The LHC at CERN

Lens Design II. Lecture 11: Further topics Herbert Gross. Winter term

CHARA Collaboration Review New York 2007 CHARA Telescope Alignment

Image Formation and Capture. Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen

Chapter 36. Image Formation

Lens Principal and Nodal Points

Limitations of lenses

Exam questions OPTI 517. Only a calculator and a single sheet of paper, 8 X11, with formulas will be allowed during the exam.

Advanced Lens Design

Tutorial Zemax 8: Correction II

Lens Design II. Lecture 11: Further topics Herbert Gross. Winter term

Physics 142 Lenses and Mirrors Page 1. Lenses and Mirrors. Now for the sequence of events, in no particular order. Dan Rather

Average: Standard Deviation: Max: 99 Min: 40

Tutorial Zemax 3 Aberrations

Converging Lenses. Parallel rays are brought to a focus by a converging lens (one that is thicker in the center than it is at the edge).

Image Formation: Camera Model

Optical Design with Zemax for PhD

Ron Liu OPTI521-Introductory Optomechanical Engineering December 7, 2009

Cameras, lenses and sensors

Lens Design I. Lecture 10: Optimization II Herbert Gross. Summer term

Cardinal Points of an Optical System--and Other Basic Facts

Transcription:

AST2210 - Lab exercise: aberrations 1 Introduction This lab exercise will take you through the most common types of aberrations. 2 Chromatic aberration Chromatic aberration causes lens to have dierent foci for dierent wavelengths. Exercise 1 Make a simple drawing illustrating chromatic aberration. We will use the set-up with the white light lamp, the color camera with microscope objective and a thin singlet lens. We have used this set-up in the rst lab exercise (CCD) this time you have to make the set-up and align the optics. You can use the ber laser the align the optics (note to use the cover on the camera!). Exercise 2 Measure the distance between the red, green, and blue foci. Take an image of each focus for your report. Exercise 3 Do you see an Airy pattern? Explain. Put a color lter in the white light lamp and explain what you see. 3 Seidel aberrations The ve Seidel aberrations are named after the German Philip Ludwig von Seidel (18211896) who decomposed the rst order monochromatic aberrations into ve constituent aberrations. They are: spherical aberration, coma, astigmatism, eld curvature, and distortion. 1

3.1 Spherical aberration Spherical aberration is caused by the eect of annuli of a lens that are of dierent radii have dierent focal lengths. See gure 1. Spherical aberration occurs in every spherical lens (and mirror), and is the only monochromatic aberration that is still present when the light beam is parallel to the optical axis. We use the same set-up as the previous exercise with the same thin singlet lens and color camera, but now with the laser connected to the collimator tube (with dampening lter). The reason for using a singlet lens is that it has more spherical aberration than doublet lenses. Doublet lenses are designed to reduce spherical aberration almost to zero. Exercise 4 Take images of the Airy pattern 1) in focus, 2) inside focus, and 3) outside focus. Explain the dierences. 3.2 Coma Coma is an aberration which causes rays from an o-axis point of light in the object plane to create a trailing "comet-like" blur directed away from the optical axis. See gure 2. The further o-axis, the worse this eect is. Coma is a serious aberration that one should try to avoid in a optical system. Nowadays it is hard to nd lenses that have signicant amount of coma. To demonstrate coma we have a specially designed lens compound. Exercise 5 Put the lens compound in the set-up with the laser, collimator tube with dampening lter and mono-chromatic camera. Tilt the lens to get various amount of coma and record images for your report. Exercise 6 Use the circular aperture to decrease the aperture. Describe what happens to the pattern. 3.3 Astigmatism Astigmatism is an aberration for which in the case of an o-axis object, rays in dierent planes have dierent foci. The planes to consider are the tangential plane: the plane containing the object and the optical axis, and the sagittal plane: the plane perpendicular to the tangential plane. See the top panel in 2

Figure 1: Spherical aberration 3

Figure 2: Dierent amounts of coma gure 3. A point source in a system with astigmatism becomes a cross, see the bottom panel of gure 3. To illustrate astigmatism, we use a thick doublet lens in the set-up with the laser, collimator tube with dampening lter and mono-chromatic camera. Exercise 7 Tilt the lens to get various amount of astigmatism and record images for your report. 3.4 Barrel/pincushion distortion When a lens suers from barrel or pincushion distortion, the magnication decreases or increases with distance from the optical axis respectively. At the present time we only have a lens with barrel distortion. The lens is directly attached to a camera, using an adapter between the lens and the camera screw the lens halfway into the adapter and then screw the adapter into the camera until a desired object in the room is focussed. Note that there is no end-stop for the lens in the adapter and there is a risk that one damages the camera sensor if one screws the lens too far into the camera. Exercise 7 Record images to illustrate barrel distortion for your report. 4 Report The report should contain the recorded images taken throughout the exercises, background to the exercises, comments on the results (the dierent kind of aberrations etc.) and explanations of the various optical setups used. 4

Figure 3: Astigmatism. Top: Rays in the tangential plane are marked with red and have their focus in T 1, rays in the sagittal plane are blue and have their focus in S 1. Bottom: point source images from an optical system with astigmatism. 5