Lens Design II. Lecture 8: Special correction topics Herbert Gross. Winter term
|
|
- Bernard Shawn Gardner
- 5 years ago
- Views:
Transcription
1 Lens Design II Lecture 8: Special correction topics Herbert Gross Winter term
2 2 Preliminary Schedule Lens Design II Aberrations and optimization Repetition Structural modifications Zero operands, lens splitting, lens addition, lens removal, material selection Aspheres Correction with aspheres, Forbes approach, optimal location of aspheres, several aspheres Freeforms Freeform surfaces, general aspects, surface description, quality assessment, initial systems Field flattening Astigmatism and field curvature, thick meniscus, plus-minus pairs, field lenses Chromatical correction I Achromatization, axial versus transversal, glass selection rules, burried surfaces Chromatical correction II Secondary spectrum, apochromatic correction, aplanatic achromates, spherochromatism Special correction topics I Symmetry, wide field systems, stop position, vignetting Special correction topics II Telecentricity, monocentric systems, anamorphotic lenses, Scheimpflug systems Higher order aberrations High NA systems, broken achromates, induced aberrations Further topics Sensitivity, scan systems, eyepieces Mirror systems special aspects, double passes, catadioptric systems Zoom systems Mechanical compensation, optical compensation Diffractive elements Color correction, ray equivalent model, straylight, third order aberrations, manufacturing
3 3 Contents 1. Symmetry 2. Camera lenses 3. Stop position 4. Vignetting
4 4 Even Aberrations in Symmetrical Systems Aberrations with even symmetry are doubled Spherical aberration, Astigmatism, field curvature, axial chromatical aberration spherical aberration in an symmetrical system W c4 Z4 c9 Z9 W c4 Z4 c9 Z9 doubled values W 2c Z 2c Z Ref: M. Seesselberg
5 5 Odd Aberrations in Symmetrical Systems Aberrations with odd symmetry are vanishing Coma, distortion, transverse chromatical aberration coma in an symmetrical system W c8 Z8 c15 Z15 W c8 Z8 c15 Z15 vanishing values Ref: M. Seesselberg W 0
6 6 Photographic lens Incidence angles for chief and marginal ray Photographic lens Field dominant system Primary goal is to control and correct field related aberrations: coma, astigmatism, field curvature, lateral color chief ray 60 incidence angle marginal ray
7 7 Principle of Symmetry Perfect symmetrical system: magnification m = -1 Stop in centre of symmetry Symmetrical contributions of wave aberrations are doubled (spherical) Asymmetrical contributions of wave aberration vanishes W(-x) = -W(x) Easy correction of: coma, distortion, chromatical change of magnification front part rear part 2 1 3
8 8 Symmetrical Dublet Variable focal length f = mm Invariant: object size y = 10 mm numerical aperture NA = 0.1 Type of system changes: - dominant spherical for large f - dominant field for small f Data: f = 200 mm f = 100 mm f = 50 mm f = 20 mm No focal length [mm] Length [mm] spherical c 9 field curvature c 4 astigmatism c f = 15 mm
9 9 Wide Angle Lenses - Symmetrical Radii of curvature of wide angle camera lenses - symmetrical setups Mostly radii 'concentric' towards the stop losition Locations z j of surfaces normalized for comparison Nearly linear trend, some exceptions near to the pupil Stop position centered R j Pleogon Double Gauss Biogon stop z j z j
10 10 Wide Angle Lenses - Asymmetrical Radii of curvature of wide angle camera lenses - asymmetrical setups No clear trend Locations z j of surfaces normalized for comparison Stop position in the rear part R j 300 Flektogon Fisheye Distagon stop z j
11 11 Coma Correction: Symmetry Principle Perfect coma correction in the case of symmetry But magnification m = -1 not useful in most practical cases Image height: y = 19 mm Symmetry principle Pupil section: meridional sagittal Transverse Aberration: y' 0.5 mm y' 0.5 mm (a) (b) From : H. Zügge
12 12 Coma Correction: Stop Position and Aspheres Combined effect, aspherical case prevent correction Plano-convex element exhibits spherical aberration Sagittal coma y' 0.5 mm Spherical aberration corrected with aspheric surface aspheric Sagittal coma y' 0.5 mm aspheric aspheric Ref : H. Zügge
13 Classification Extrem Wide Angle Fish Eye Quasi-Symmetrical Angle Topogon Metrogon Special Telecentric I Families of photographic lenses Long history Not unique Panoramic Lens Pleon Wide Angle Retrofocus Retrofocus SLR Super-Angulon Pleogon Hypergon Hologon Telephoto Plastic Aspheric I Telecentric II Compact Catadioptric Plastic Aspheric II Flektogon Distagon Biogon IR Camera Lens UV Lens Triplets Retrofocus II Vivitar Triplet Pentac Ernostar Less Symmetrical Ernostar II Landscape Singlets Achromatic Landscape Heliar Hektor Inverse Triplet Sonnar Double Gauss Biotar / Planar Quadruplets Ultran Petzval, Portrait Petzval Petzval,Portrait flat Petzval Projection R-Biotar Symmetrical Doublets Dagor Dagor reversed Rapid Rectilinear Aplanat Periskop Double Gauss II Noctilux Quasi-Symmetrical Doublets Tessar Protar Orthostigmatic Plasmat Kino-Plasmat Celor Unar Antiplanet Angulon
14 14 Symmetry Principle Application of symmetry principle: photographic lenses Especially field dominant aberrations can be corrected Also approximate fulfillment of symmetry condition helps Triplet significantly: quasi symmetry Realization of quasisymmetric setups in nearly all photographic systems Double Gauss (6 elements) Biogon Double Gauss (7 elements) Ref : H. Zügge
15 Photographic Lenses Tessar Distagon Double Gauss Tele system Super Angulon Wide angle Fish-eye
16 Retrofocus Lenses Example lens 2 Distagon
17 Special Designs Compact Camera Plastic Aspheric Lens Mobile Phone camera
18 Handy Phone Objective lenses Examples US L = 4.2 mm, F'=2.8, f = 3.67 mm, 2w=2x34 US L = 6.0 mm, F'=2.8, f = 4.0 mm, 2w=2x31 EP L = 5.37 mm, F'=2.88, f = 3.32 mm, 2w=2x33.9 Olympus 2 L = 7.5 mm, F'=2.8, f = 4.57 mm, 2w=2x33 Ref: T. Steinich
19 Fish-Eye-Lens Nikon 210 Pleon (air reconnaissance)
20 Wide-Angle Lenses Hypergon Strong vignetting 1.0 I(r) 0.5 Topogon Metrogon field 0 angle w
21 Wide-Angle Lenses Hologon Inverse Triplet Pleogon Biogon Super-Angulon
22 Retrofocus Lenses Flektogon Vivitar
23 Fish-Eye-Lens Example lens fisheye y -100% 0 100% a) nm 587 nm 656 nm tan sag ideal [mm -1 ] cyc/mm 20 cyc/mm 40 cyc/mm 60 cyc/mm b) c) solid: tan dashed: sag field angle 100
24 Fish-Eye-Lens Pupil variation: position and orientation pupil location s ExP [mm] 110 a y' ExP [mm] 150 b w [ ] w [ ]
25 Fish-Eye-Lens Distortion types y' [a.u.] 2 gnomonic stereographic 1.5 f- -projection orthographic y' [mm] 1 aperture related y' = f' tan(w) y' = f' w fisheye lens w [ ] 10 a b w [ ]
26 26 Optimization of the Stop Position Change of stop position changes the path of the ray bundle for the field points through the system Aberrations changes Vignetting occur for extrem pupil positions
27 27 Stop Shift Formula exit pupil semi diameter h E T T h H field height h E εh H ρ ε Normalized field height Normalized pupil height Stop shift parameter T old exit pupil T new exit pupil image plane Taylor series expansion using stop shift parameter: Examples: W spherical aberration W new ρ; H = W old ρ x, ρ y + εh; H = W old ρ; H + εh ρy W old ρ; H + ε2 2 H2 2 ρy W old ρ; H + constant spherical aberration linear coma quadratic astigmatism & curvature W coma linear coma quadratic astigmatism & curvature cubic distortion Ref: D. Ochse
28 28 Optimization of the Stop Position Relay system Change of stop size and position without re-optimization: 1. Vignetting occurs 2. Performance drops spot size in mm relative illumination NA optimized point NA optimized point z-enp z-enp
29 29 Optimization of the Stop Position Relay system Change of stop position with re-optimization: 1. Vignetting occurs 2. Performance drops In case of vignetting: spot size grows more slowly Optimal stop position inside the system due to averaged chief ray heights D spot in mm transmission 1 no vignetting without vignetting z-pupil z-pupil
30 30 Influence of Stop Position on Performance Ray path of chief ray depends on stop position stop positions spot
31 31 Stop Position Relative stop position in wide angle camera lenses: - symmetric / asymmetric concepts - angle ratio incoming / outgoing balanced - relative chief ray heights balanced / diameters - chief ray correction - special case aspheres Fisheye lens w inc = 85 w out = 7 Super Angulon w inc = 45 w out = 48 Handy lens II aspheres w inc = 34 w out = 22 Flektogon w inc = 45 w out = 25 Pleogon w inc = 45 w out = 46 Handy lens I aspheres w inc = 33 w out = 34 Distagon I w inc = 37 w out = 21 Distagon I w inc = 27 w out = -3
32 32 Effect of Stop Position Example photographic lens stop Small axial shift of stop changes tranverse aberrations In particular coma is strongly influenced Ref: H.Zügge
33 33 Aberrations Limited by Vignetting Clipping of outer coma rays by vignetting Consequences: - reduced brightness - anisotropic resolution without vignettierung with vignettierung tangential / sagittal Ref: H.Zügge
34 34 Vignetting Double Gauss Lens 1.4 / 50 Improved performance Reduced uniformity of brightness a) no vignetting:weight 251 g relative illumination b) vignetted: weight 90 g 81 % F# 2.8 Ref.: H. Zügge
Lens Design II. Lecture 8: Special correction features I Herbert Gross. Winter term
Lens Design II Lecture 8: Special correction features I 2015-12-08 Herbert Gross Winter term 2015 www.iap.uni-jena.de Preliminary Schedule 2 1 20.10. Aberrations and optimization Repetition 2 27.10. Structural
More informationLens Design II. Lecture 8: Special correction features I Herbert Gross. Winter term
Lens Design II Lecture 8: Special correction features I 2017-12-04 Herbert Gross Winter term 2017 www.iap.uni-jena.de 2 Preliminary Schedule Lens Design II 2017 1 16.10. Aberrations and optimization Repetition
More informationLens Design II. Lecture 2: Structural modifications Herbert Gross. Winter term
Lens Design II Lecture 2: Structural modifications 26--26 Herbert Gross Winter term 26 www.iap.uni-jena.de 2 Preliminary Schedule 9.. Aberrations and optimization Repetition 2 26.. Structural modifications
More informationAdvanced Lens Design
Advanced Lens Design Lecture 3: Aberrations I 214-11-4 Herbert Gross Winter term 214 www.iap.uni-jena.de 2 Preliminary Schedule 1 21.1. Basics Paraxial optics, imaging, Zemax handling 2 28.1. Optical systems
More informationLens Design II. Lecture 11: Further topics Herbert Gross. Winter term
Lens Design II Lecture : Further topics 28--8 Herbert Gross Winter term 27 www.iap.uni-ena.de 2 Preliminary Schedule Lens Design II 27 6.. Aberrations and optimization Repetition 2 23.. Structural modifications
More informationOptical Design with Zemax for PhD
Optical Design with Zemax for PhD Lecture 7: Optimization II 26--2 Herbert Gross Winter term 25 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed content.. Introduction 2 2.2. Basic Zemax
More informationOptical Design with Zemax
Optical Design with Zemax Lecture : Correction II 3--9 Herbert Gross Summer term www.iap.uni-jena.de Correction II Preliminary time schedule 6.. Introduction Introduction, Zemax interface, menues, file
More informationDesign and Correction of Optical Systems
Design and Correction of Optical Systems Lecture 12: Optical system classification 2017-06-30 Herbert Gross Summer term 2017 www.iap.uni-jena.de 2 Preliminary Schedule - DCS 2017 1 07.04. Basics 2 21.04.
More informationLens Design II. Lecture 11: Further topics Herbert Gross. Winter term
Lens Design II Lecture : Further topics 26--2 Herbert Gross Winter term 25 www.iap.uni-ena.de Preliminary Schedule 2 2.. Aberrations and optimization Repetition 2 27.. Structural modifications Zero operands,
More informationDesign and Correction of Optical Systems
Design and Correction of Optical Systems Lecture 12: Optical system classification 2015-07-01 Herbert Gross Summer term 2015 www.iap.uni-jena.de 2 Preliminary Schedule 1 15.04. Basics 2 22.04. Materials
More informationLens Design I. Lecture 10: Optimization II Herbert Gross. Summer term
Lens Design I Lecture : Optimization II 5-6- Herbert Gross Summer term 5 www.iap.uni-jena.de Preliminary Schedule 3.. Basics.. Properties of optical systrems I 3 7.5..5. Properties of optical systrems
More informationLens Design I. Lecture 10: Optimization II Herbert Gross. Summer term
Lens Design I Lecture : Optimization II 8-6- Herbert Gross Summer term 8 www.iap.uni-jena.de Preliminary Schedule - Lens Design I 8.4. Basics 9.4. Properties of optical systems I 3 6.4. Properties of optical
More informationTelecentric Imaging Object space telecentricity stop source: edmund optics The 5 classical Seidel Aberrations First order aberrations Spherical Aberration (~r 4 ) Origin: different focal lengths for different
More informationLens Design II. Lecture 3: Aspheres Herbert Gross. Winter term
Lens Design II Lecture 3: Aspheres 6-- Herbert Gross Winter term 6 www.iap.uni-jena.de Preliminar Schedule 9.. Aberrations and optimiation Repetition 6.. Structural modifications Zero operands, lens splitting,
More informationImaging and Aberration Theory
Imaging and Aberration Theory Lecture 7: Distortion and coma 2014-12-11 Herbert Gross Winter term 2014 www.iap.uni-jena.de 2 Preliminary time schedule 1 30.10. Paraxial imaging paraxial optics, fundamental
More informationLens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term
Lens Design I Lecture 3: Properties of optical systems II 207-04-20 Herbert Gross Summer term 207 www.iap.uni-jena.de 2 Preliminary Schedule - Lens Design I 207 06.04. Basics 2 3.04. Properties of optical
More informationLens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term
Lens Design I Lecture 3: Properties of optical systems II 205-04-8 Herbert Gross Summer term 206 www.iap.uni-jena.de 2 Preliminary Schedule 04.04. Basics 2.04. Properties of optical systrems I 3 8.04.
More informationAdvanced Lens Design
Advanced Lens Design Lecture 4: Optimization III 2013-11-04 Herbert Gross Winter term 2013 www.iap.uni-jena.de 2 Preliminary Schedule 1 15.10. Introduction Paraxial optics, ideal lenses, optical systems,
More informationLens Design I. Lecture 5: Advanced handling I Herbert Gross. Summer term
Lens Design I Lecture 5: Advanced handling I 2018-05-17 Herbert Gross Summer term 2018 www.iap.uni-jena.de 2 Preliminary Schedule - Lens Design I 2018 1 12.04. Basics 2 19.04. Properties of optical systems
More informationOptical Design with Zemax
Optical Design with Zemax Lecture : Correction I 203-0-22 Herbert Gross Summer term 202 www.iap.uni-jena.de Preliminary time schedule 2 6.0. Introduction Introduction, Zemax interface, menues, file handling,
More informationIntroduction to Optical Modeling. Friedrich-Schiller-University Jena Institute of Applied Physics. Lecturer: Prof. U.D. Zeitner
Introduction to Optical Modeling Friedrich-Schiller-University Jena Institute of Applied Physics Lecturer: Prof. U.D. Zeitner The Nature of Light Fundamental Question: What is Light? Newton Huygens / Maxwell
More informationLens Design II. Lecture 3: Aspheres Herbert Gross. Winter term
Lens Design II Lecture 3: Aspheres 7--3 Herbert Gross Winter term 7 www.iap.uni-jena.de Preliminar Schedule Lens Design II 7 6.. Aberrations and optimiation Repetition 3.. Structural modifications Zero
More informationIndex. B Back focal length, 12 Beam expander, 35 Berek, Max, 244 Binary phase grating, 326 Buried surface, 131,
About the Author The author studied Technical Physics at the Technical University of Delft, The Netherlands. He obtained a master s degree in 1965 with a thesis on the fabrication of lasers. After military
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 9: Advanced handling 2014-06-13 Herbert Gross Sommer term 2014 www.iap.uni-jena.de 2 Preliminary Schedule 1 11.04. Introduction 2 25.04. Properties of optical systems
More informationSPIE. Lens Design Fundamentals PRESS. Second Edition RUDOLF KINGSLAKE R. BARRY JOHNSON
Lens Design Fundamentals Second Edition RUDOLF KINGSLAKE R. BARRY JOHNSON AMSTERDAM BOSTON HEIDELBERG LONDON NEW YORK OXFORD PARIS SAN DIEGO SAN FRANCISCO SINGAPORE SYDNEY TOKYO Academic Press is an imprint
More informationLens Design I. Lecture 5: Advanced handling I Herbert Gross. Summer term
Lens Design I Lecture 5: Advanced handling I 2015-05-11 Herbert Gross Summer term 2015 www.iap.uni-jena.de 2 Preliminary Schedule 1 13.04. Basics 2 20.04. Properties of optical systrems I 3 27.05. Properties
More informationTutorial Zemax 8: Correction II
Tutorial Zemax 8: Correction II 2012-10-11 8 Correction II 1 8.1 High-NA Collimator... 1 8.2 Zoom-System... 6 8.3 New Achromate and wide field system... 11 8 Correction II 8.1 High-NA Collimator An achromatic
More informationSome lens design methods. Dave Shafer David Shafer Optical Design Fairfield, CT #
Some lens design methods Dave Shafer David Shafer Optical Design Fairfield, CT 06824 #203-259-1431 shaferlens@sbcglobal.net Where do we find our ideas about how to do optical design? You probably won t
More informationIntroductions to aberrations OPTI 517
Introductions to aberrations OPTI 517 Lecture 11 Spherical aberration Meridional and sagittal ray fans Spherical aberration 0.25 wave f/10; f=100 mm; wave=0.0005 mm Spherical aberration 0.5 wave f/10;
More informationDesign and Correction of optical Systems
Design and Correction of optical Sstems Part 5: Properties of Optical Sstems Summer term 2012 Herbert Gross Overview 2 1. Basics 2012-04-18 2. Materials 2012-04-25 3. Components 2012-05-02 4. Paraxial
More informationLecture 4: Geometrical Optics 2. Optical Systems. Images and Pupils. Rays. Wavefronts. Aberrations. Outline
Lecture 4: Geometrical Optics 2 Outline 1 Optical Systems 2 Images and Pupils 3 Rays 4 Wavefronts 5 Aberrations Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl Lecture 4: Geometrical
More informationLens Design II Seminar 6 (Solutions)
2017-01-04 Prof. Herbert Gross Yi Zhong, Norman G. Worku Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design II Seminar 6 (Solutions) 6.1. Correction
More informationPerformance Factors. Technical Assistance. Fundamental Optics
Performance Factors After paraxial formulas have been used to select values for component focal length(s) and diameter(s), the final step is to select actual lenses. As in any engineering problem, this
More information1.1 Singlet. Solution. a) Starting setup: The two radii and the image distance is chosen as variable.
1 1.1 Singlet Optimize a single lens with the data λ = 546.07 nm, object in the distance 100 mm from the lens on axis only, focal length f = 45 mm and numerical aperture NA = 0.07 in the object space.
More informationLecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.
Lecture 2: Geometrical Optics Outline 1 Geometrical Approximation 2 Lenses 3 Mirrors 4 Optical Systems 5 Images and Pupils 6 Aberrations Christoph U. Keller, Leiden Observatory, keller@strw.leidenuniv.nl
More informationLecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.
Lecture 2: Geometrical Optics Outline 1 Geometrical Approximation 2 Lenses 3 Mirrors 4 Optical Systems 5 Images and Pupils 6 Aberrations Christoph U. Keller, Leiden Observatory, keller@strw.leidenuniv.nl
More informationGEOMETRICAL OPTICS AND OPTICAL DESIGN
GEOMETRICAL OPTICS AND OPTICAL DESIGN Pantazis Mouroulis Associate Professor Center for Imaging Science Rochester Institute of Technology John Macdonald Senior Lecturer Physics Department University of
More informationExercise 1 - Lens bending
Exercise 1 - Lens bending Most of the aberrations change with the bending of a lens. This is demonstrated in this exercise. a) Establish a lens with focal length f = 100 mm made of BK7 with thickness 5
More informationLens Design I Seminar 1
Xiang Lu, Ralf Hambach Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design I Seminar 1 Warm-Up (20min) Setup a single, symmetric, biconvex lens
More informationOPTICAL IMAGING AND ABERRATIONS
OPTICAL IMAGING AND ABERRATIONS PARTI RAY GEOMETRICAL OPTICS VIRENDRA N. MAHAJAN THE AEROSPACE CORPORATION AND THE UNIVERSITY OF SOUTHERN CALIFORNIA SPIE O P T I C A L E N G I N E E R I N G P R E S S A
More informationExam questions OPTI 517. Only a calculator and a single sheet of paper, 8 X11, with formulas will be allowed during the exam.
Exam questions OPTI 517 Only a calculator an a single sheet of paper, 8 X11, with formulas will be allowe uring the exam. 1) A single optical spherical surface oes not contribute spherical aberration.
More informationExam Preparation Guide Geometrical optics (TN3313)
Exam Preparation Guide Geometrical optics (TN3313) Lectures: September - December 2001 Version of 21.12.2001 When preparing for the exam, check on Blackboard for a possible newer version of this guide.
More informationSequential Ray Tracing. Lecture 2
Sequential Ray Tracing Lecture 2 Sequential Ray Tracing Rays are traced through a pre-defined sequence of surfaces while travelling from the object surface to the image surface. Rays hit each surface once
More informationMicroscopy. Lecture 2: Optical System of the Microscopy II Herbert Gross. Winter term
Microscopy Lecture 2: Optical System of the Microscopy II 212-1-22 Herbert Gross Winter term 212 www.iap.uni-jena.de Preliminary time schedule 2 No Date Main subject Detailed topics Lecturer 1 15.1. Optical
More informationOptical Design with Zemax for PhD - Basics
Optical Design with Zemax for PhD - Basics Lecture 3: Properties of optical sstems II 2013-05-30 Herbert Gross Summer term 2013 www.iap.uni-jena.de 2 Preliminar Schedule No Date Subject Detailed content
More informationLong Wave Infrared Scan Lens Design And Distortion Correction
Long Wave Infrared Scan Lens Design And Distortion Correction Item Type text; Electronic Thesis Authors McCarron, Andrew Publisher The University of Arizona. Rights Copyright is held by the author. Digital
More informationWarren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California
Modern Optical Engineering The Design of Optical Systems Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California Fourth Edition Me Graw Hill New York Chicago San Francisco
More informationThe Brownie Camera. Lens Design OPTI 517. Prof. Jose Sasian
The Brownie Camera Lens Design OPTI 517 http://www.history.roch ester.edu/class/kodak/k odak.htm George Eastman (1854-1932), was an ingenious man who contributed greatly to the field of photography. He
More informationIntroduction. Geometrical Optics. Milton Katz State University of New York. VfeWorld Scientific New Jersey London Sine Singapore Hong Kong
Introduction to Geometrical Optics Milton Katz State University of New York VfeWorld Scientific «New Jersey London Sine Singapore Hong Kong TABLE OF CONTENTS PREFACE ACKNOWLEDGMENTS xiii xiv CHAPTER 1:
More informationINTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS
INTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS JOSE SASIÄN University of Arizona ШШ CAMBRIDGE Щ0 UNIVERSITY PRESS Contents Preface Acknowledgements Harold H. Hopkins Roland V. Shack Symbols 1 Introduction
More informationCHAPTER 33 ABERRATION CURVES IN LENS DESIGN
CHAPTER 33 ABERRATION CURVES IN LENS DESIGN Donald C. O Shea Georgia Institute of Technology Center for Optical Science and Engineering and School of Physics Atlanta, Georgia Michael E. Harrigan Eastman
More informationApplied Optics. , Physics Department (Room #36-401) , ,
Applied Optics Professor, Physics Department (Room #36-401) 2290-0923, 019-539-0923, shsong@hanyang.ac.kr Office Hours Mondays 15:00-16:30, Wednesdays 15:00-16:30 TA (Ph.D. student, Room #36-415) 2290-0921,
More informationOptimisation. Lecture 3
Optimisation Lecture 3 Objectives: Lecture 3 At the end of this lecture you should: 1. Understand the use of Petzval curvature to balance lens components 2. Know how different aberrations depend on field
More informationOptical System Design
Phys 531 Lecture 12 14 October 2004 Optical System Design Last time: Surveyed examples of optical systems Today, discuss system design Lens design = course of its own (not taught by me!) Try to give some
More informationLaboratory experiment aberrations
Laboratory experiment aberrations Obligatory laboratory experiment on course in Optical design, SK2330/SK3330, KTH. Date Name Pass Objective This laboratory experiment is intended to demonstrate the most
More informationGeometric optics & aberrations
Geometric optics & aberrations Department of Astrophysical Sciences University AST 542 http://www.northerneye.co.uk/ Outline Introduction: Optics in astronomy Basics of geometric optics Paraxial approximation
More informationExercises Advanced Optical Design Part 5 Solutions
2014-12-09 Manuel Tessmer M.Tessmer@uni-jena.dee Minyi Zhong minyi.zhong@uni-jena.de Herbert Gross herbert.gross@uni-jena.de Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str.
More informationTutorial Zemax Introduction 1
Tutorial Zemax Introduction 1 2012-07-17 1 Introduction 1 1.1 Exercise 1-1: Stair-mirror-setup... 1 1.2 Exercise 1-2: Symmetrical 4f-system... 5 1 Introduction 1.1 Exercise 1-1: Stair-mirror-setup Setup
More informationSome of the important topics needed to be addressed in a successful lens design project (R.R. Shannon: The Art and Science of Optical Design)
Lens design Some of the important topics needed to be addressed in a successful lens design project (R.R. Shannon: The Art and Science of Optical Design) Focal length (f) Field angle or field size F/number
More informationOptical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics
Optical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics 1011CE Restricts rays: acts as a single lens: inverts
More informationGeometrical Optics Optical systems
Phys 322 Lecture 16 Chapter 5 Geometrical Optics Optical systems Magnifying glass Purpose: enlarge a nearby object by increasing its image size on retina Requirements: Image should not be inverted Image
More informationME 297 L4-2 Optical design flow Analysis
ME 297 L4-2 Optical design flow Analysis Nayer Eradat Fall 2011 SJSU 1 Are we meeting the specs? First order requirements (after scaling the lens) Distortion Sharpness (diffraction MTF-will establish depth
More informationPhotographic zoom fisheye lens design for DSLR cameras
Photographic zoom fisheye lens design for DSLR cameras Yufeng Yan Jose Sasian Yufeng Yan, Jose Sasian, Photographic zoom fisheye lens design for DSLR cameras, Opt. Eng. 56(9), 095103 (2017), doi: 10.1117/1.OE.56.9.095103.
More informationCOURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR)
COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR) PAPER TITLE: BASIC PHOTOGRAPHIC UNIT - 3 : SIMPLE LENS TOPIC: LENS PROPERTIES AND DEFECTS OBJECTIVES By
More informationOptical design of a high resolution vision lens
Optical design of a high resolution vision lens Paul Claassen, optical designer, paul.claassen@sioux.eu Marnix Tas, optical specialist, marnix.tas@sioux.eu Prof L.Beckmann, l.beckmann@hccnet.nl Summary:
More informationLenses Design Basics. Introduction. RONAR-SMITH Laser Optics. Optics for Medical. System. Laser. Semiconductor Spectroscopy.
Introduction Optics Application Lenses Design Basics a) Convex lenses Convex lenses are optical imaging components with positive focus length. After going through the convex lens, parallel beam of light
More informationWaves & Oscillations
Physics 42200 Waves & Oscillations Lecture 33 Geometric Optics Spring 2013 Semester Matthew Jones Aberrations We have continued to make approximations: Paraxial rays Spherical lenses Index of refraction
More informationMedical Photonics Lecture 1.2 Optical Engineering
Medical Photonics Lecture 1.2 Optical Engineering Lecture 9: Instruments I 2016-12-15 Michael Kempe Winter term 2016 www.iap.uni-jena.de 2 Contents No Subject Ref Date Detailed Content 1 Introduction Gross
More informationECEG105/ECEU646 Optics for Engineers Course Notes Part 4: Apertures, Aberrations Prof. Charles A. DiMarzio Northeastern University Fall 2008
ECEG105/ECEU646 Optics for Engineers Course Notes Part 4: Apertures, Aberrations Prof. Charles A. DiMarzio Northeastern University Fall 2008 July 2003+ Chuck DiMarzio, Northeastern University 11270-04-1
More informationOptical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember
Günter Toesko - Laserseminar BLZ im Dezember 2009 1 Aberrations An optical aberration is a distortion in the image formed by an optical system compared to the original. It can arise for a number of reasons
More informationSupplemental Materials. Section 25. Aberrations
OTI-201/202 Geometrical and Instrumental Optics 25-1 Supplemental Materials Section 25 Aberrations Aberrations of the Rotationally Symmetric Optical System First-order or paraxial systems are ideal optical
More informationOptical Zoom System Design for Compact Digital Camera Using Lens Modules
Journal of the Korean Physical Society, Vol. 50, No. 5, May 2007, pp. 1243 1251 Optical Zoom System Design for Compact Digital Camera Using Lens Modules Sung-Chan Park, Yong-Joo Jo, Byoung-Taek You and
More informationUsing molded chalcogenide glass technology to reduce cost in a compact wide-angle thermal imaging lens
Using molded chalcogenide glass technology to reduce cost in a compact wide-angle thermal imaging lens George Curatu a, Brent Binkley a, David Tinch a, and Costin Curatu b a LightPath Technologies, 2603
More informationCardinal Points of an Optical System--and Other Basic Facts
Cardinal Points of an Optical System--and Other Basic Facts The fundamental feature of any optical system is the aperture stop. Thus, the most fundamental optical system is the pinhole camera. The image
More informationLenses, exposure, and (de)focus
Lenses, exposure, and (de)focus http://graphics.cs.cmu.edu/courses/15-463 15-463, 15-663, 15-862 Computational Photography Fall 2017, Lecture 15 Course announcements Homework 4 is out. - Due October 26
More informationUsing Stock Optics. ECE 5616 Curtis
Using Stock Optics What shape to use X & Y parameters Please use achromatics Please use camera lens Please use 4F imaging systems Others things Data link Stock Optics Some comments Advantages Time and
More informationCh 24. Geometric Optics
text concept Ch 24. Geometric Optics Fig. 24 3 A point source of light P and its image P, in a plane mirror. Angle of incidence =angle of reflection. text. Fig. 24 4 The blue dashed line through object
More informationThe Basic Scheme of the Afocal System and Composition Variants of the Objectives Based on It
Journal of Physics: Conference Series The Basic Scheme of the Afocal System and Composition Variants of the Objectives Based on It To cite this article: Gavriluk A V et al 006 J. Phys.: Conf. Ser. 48 945
More informationSolution of Exercises Lecture Optical design with Zemax for PhD Part 8
2013-06-17 Prof. Herbert Gross Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Solution of Exercises Lecture Optical design with Zemax for PhD Part 8 8.1
More informationCHAPTER 1 Optical Aberrations
CHAPTER 1 Optical Aberrations 1.1 INTRODUCTION This chapter starts with the concepts of aperture stop and entrance and exit pupils of an optical imaging system. Certain special rays, such as the chief
More informationHandbook of Optical Systems
Handbook of Optical Systems Edited by Herbert Gross Volume 3: Aberration Theory and Correction of Optical Systems Herbert Cross, Hannfried Zügge, Martin Peschka, Fritz Blechinger BICENTENNIAL BICENTENNIA
More informationOpti 415/515. Introduction to Optical Systems. Copyright 2009, William P. Kuhn
Opti 415/515 Introduction to Optical Systems 1 Optical Systems Manipulate light to form an image on a detector. Point source microscope Hubble telescope (NASA) 2 Fundamental System Requirements Application
More informationLens Design I Seminar 5
Y. Sekman, X. Lu, H. Gross Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design I Seminar 5 Exercise 5-1: PSF scaling (Homework) To check the Airy
More informationLithography Smash Sensor Objective Product Requirements Document
Lithography Smash Sensor Objective Product Requirements Document Zhaoyu Nie (Project Manager) Zichan Wang (Customer Liaison) Yunqi Li (Document) Customer: Hong Ye (ASML) Faculty Advisor: Julie Bentley
More informationAstro 500 A500/L-8! 1!
Astro 500 1! Optics! Review! Compound systems: Outline o Pupils, stops, and telecentricity Telescopes! Review! Two-mirror systems! Figures of merit Examples: WIYN & SALT 2! Review: The Thin Lens! s parallel
More informationLenses. Overview. Terminology. The pinhole camera. Pinhole camera Lenses Principles of operation Limitations
Overview Pinhole camera Principles of operation Limitations 1 Terminology The pinhole camera The first camera - camera obscura - known to Aristotle. In 3D, we can visualize the blur induced by the pinhole
More informationChapter 34 Geometric Optics (also known as Ray Optics) by C.-R. Hu
Chapter 34 Geometric Optics (also known as Ray Optics) by C.-R. Hu 1. Principles of image formation by mirrors (1a) When all length scales of objects, gaps, and holes are much larger than the wavelength
More informationTOPICS Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization
TOPICS Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization Lens Aberrations - 3 lectures Spherical aberrations Coma, astigmatism,
More informationEE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name:
EE119 Introduction to Optical Engineering Spring 2002 Final Exam Name: SID: CLOSED BOOK. FOUR 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental
More informationj Jacobi matrix 295 Index flattening mirror 258 flint glass 231 form tolerance 598, 605 ff free-form aspheres 456 Fresnel zone plate 499, 503 f
749 a Abbe number 41, 222, 269, 490, 502 aberrations 2, 216 astigmatism 13, 28 axial chromatic aberration 13, 269 axial color 13, 269 chromatic aberrations 2, 13, 187, 268, 280 chromatic difference in
More informationReflection! Reflection and Virtual Image!
1/30/14 Reflection - wave hits non-absorptive surface surface of a smooth water pool - incident vs. reflected wave law of reflection - concept for all electromagnetic waves - wave theory: reflected back
More informationChapter 3. Introduction to Zemax. 3.1 Introduction. 3.2 Zemax
Chapter 3 Introduction to Zemax 3.1 Introduction Ray tracing is practical only for paraxial analysis. Computing aberrations and diffraction effects are time consuming. Optical Designers need some popular
More informationOSLO Doublet Optimization Tutorial
OSLO Doublet Optimization Tutorial This tutorial helps optical designers with the most basic process for setting up a lens and optimizing in OSLO. The example intentionally goes through basics as well
More informationOPAC 202 Optical Design and Inst.
OPAC 202 Optical Design and Inst. Topic 9 Aberrations Department of http://www.gantep.edu.tr/~bingul/opac202 Optical & Acustical Engineering Gaziantep University Apr 2018 Sayfa 1 Introduction The influences
More informationOPTICAL SYSTEMS OBJECTIVES
101 L7 OPTICAL SYSTEMS OBJECTIVES Aims Your aim here should be to acquire a working knowledge of the basic components of optical systems and understand their purpose, function and limitations in terms
More informationWhy is There a Black Dot when Defocus = 1λ?
Why is There a Black Dot when Defocus = 1λ? W = W 020 = a 020 ρ 2 When a 020 = 1λ Sag of the wavefront at full aperture (ρ = 1) = 1λ Sag of the wavefront at ρ = 0.707 = 0.5λ Area of the pupil from ρ =
More informationDesign of Large Working Area F-Theta Lens. Gong Chen
1 Design of Large Working Area F-Theta Lens by Gong Chen 2 ABSTRACT F-Theta lenses are different from normal camera lenses. It is one of the most important parts of laser scanning system. Besides, F-Theta
More informationSolution of Exercises Lecture Optical design with Zemax Part 6
2013-06-17 Prof. Herbert Gross Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Solution of Exercises Lecture Optical design with Zemax Part 6 6 Illumination
More informationChapter B.3. The Cooke Triplet and Tessar Lenses
Chapter B.3 The Cooke Triplet and Tessar Lenses (Entire contents Copyright c 1998 by Gregory Hallock Smith, All Rights Reserved) Following the introduction of photography in 1839, the development of camera
More informationAstronomy 80 B: Light. Lecture 9: curved mirrors, lenses, aberrations 29 April 2003 Jerry Nelson
Astronomy 80 B: Light Lecture 9: curved mirrors, lenses, aberrations 29 April 2003 Jerry Nelson Sensitive Countries LLNL field trip 2003 April 29 80B-Light 2 Topics for Today Optical illusion Reflections
More information