Lens Design I. Lecture 1: Basics Herbert Gross. Summer term
|
|
- Derek Maxwell
- 5 years ago
- Views:
Transcription
1 Lens Design I Lecture 1: Basics Herbert Gross Summer term
2 2 Preliminary Schedule Basics Properties of optical systems I Properties of optical systems II Properties of optical systems III Introduction, Zemax interface, menues, file handling, preferences, Editors, updates, windows, coordinates, System description, 3D geometry, aperture, field, wavelength Diameters, stop and pupil, vignetting, Layouts, Materials, Glass catalogs, Raytrace, Ray fans and sampling, Footprints Types of surfaces, cardinal elements, lens properties, Imaging, magnification, paraxial approximation and modelling, telecentricity, infinity object distance and afocal image, local/global coordinates Component reversal, system insertion, scaling of systems, aspheres, gratings and diffractive surfaces, gradient media, solves Advanced handling I Miscellaneous, fold mirror, universal plot, slider, multiconfiguration, lens catalogs Aberrations I Representation of geometrical aberrations, Spot diagram, Transverse aberration diagrams, Aberration expansions, Primary aberrations Aberrations II Wave aberrations, Zernike polynomials, measurement of quality Aberrations III Point spread function, Optical transfer function Optimization I Optimization II Advanced handling II Principles of nonlinear optimization, Optimization in optical design, general process, optimization in Zemax Initial systems, special issues, sensitivity of variables in optical systems, global optimization methods System merging, ray aiming, moving stop, double pass, IO of data, material index fit, stock lens matching, macro language Correction I Correction II Symmetry principle, lens bending, correcting spherical aberration, coma, astigmatism, field curvature, chromatical correction Field lenses, stop position influence, retrofocus and telephoto setup, aspheres and higher orders, freeform systems, miscellaneous
3 3 Contents 1 st Lecture 1. Introduction 2. Zemax interface, menues, file handling, preferences 3. Editors, updates, windows 4. Coordinate systems and notations 5. Aperture, field, wavelength 6. System description 7. 3D geometry
4 4 Modelling of Optical Systems Principal purpose of calculations: Imaging model with levels of refinement System, data of the structure (radii, distances, indices,...) Analysis imaging aberration theorie Synthesis lens design Function, data of properties, quality performance (spot diameter, MTF, Strehl ratio,...) Paraxial model (focal length, magnification, aperture,..) linear approximation Analytical approximation and classification (aberrations,..) Taylor expansion Geometrical optics (transverse aberrations, wave aberration, distortion,...) with diffraction approximation --> 0 Wave optics (point spread function, OTF,...) Ref: W. Richter
5 5 Modelling of Optical Systems Five levels of modelling: 1. Geometrical raytrace with analysis 2. Equivalent geometrical quantities, classification 3. Physical model: complex pupil function 4. Primary physical quantities 5. Secondary physical quantities Blue arrows: conversion of quantities Geometrical raytrace with Snells law Geometrical equivalents classification Physical model Primary physical quantities Secondary physical quantities ray tracing intersection points optical path length reference sphere wave aberration W exponential function of the phase pupil function Kirchhoff integral integration autocorrelation Duffieux integral orthogonal expansion optical transfer function approximation diameter of the spot Zernike coefficients Fourier transform Luneburg integral ( far field ) point spread function (PSF) maximum of the squared amplitude Fourier transform squared amplitude Rayleigh unit equivalence types of aberrations longitudinal aberrations final analysis reference ray in the image space Strehl number approximation threshold value spatial frequency resolution analysis sum of coefficients Marechal approximation sum of squares Marechal approximation rms value integration of spatial frequencies geometrical optical transfer function transverse aberration differen tiation definition single types of aberrations Marechal approximation final analysis reference ray in the image plane full aperture geometrical spot diagramm Fourier transform threshold value spatial frequency approximation spot diameter
6 6 Zemax Interface There are 4 types of windows in Zemax: 1. Editors for data input: lens data, extra data, multiconfiguration, tolerances 2. Output windows for graphical representation of results Here mostly setting-windowss are supported to optimize the layout 3. Text windows for output in ASCII numerical numbers (can be exported) 4. Dialog boxes for data input, error reports and more There are several files associates with Zemax 1. Data files (.ZMX) 2. Session files (.SES) for system settings (can be de-activated) 3. Glass catalogs, lens catalogs, coating catalogs, BRDF catalogs, macros, images, POP data, refractive index files,... There are in general two working modes of Zemax 1. Sequential raytrace (or partial non-sequencial) 2. Non-sequential
7 7 Coordinate Systems and Sign of Quantities Coordinate systems 2D sections: y-z shown y / meridional section tangential plane x / sagittal plane Sign of lengths, radii, angles: z / optical axis - s + s - R 2 + R 1 negative: to the left positive: + R to the right C 2 positive: C to the right negative: C to the left C 1 + j angle positive: counterclockwise reference
8 8 Description of Optical Systems Interface surfaces - mathematical modelled surfaces - planes, spheres, aspheres, conics, free shaped surfaces, Size of components - thickness and distances along the axis - transversal size,circular diameter, complicated contours Geometry of the setup - special case: rotational symmetry - general case: 3D, tilt angles, offsets and decentrations, needs vectorial approach Materials - refractive indices for all used wavelengths - other properties: absorption, birefringence, nonlinear coefficients, index gradients, Special surfaces - gratings, diffractive elements - arrays, scattering surfaces
9 9 System Model Single step: - surface and transition - parameters: radius, diameter, thickness, refractive index, aspherical constants, conic parameter, decenter, tilt,... diameter D j surface j medium j t j / n j radius r j Complete system: - sequence of surfaces - object has index 0 - image has index N - tn does not exist Ray path has fixed sequence (N-1)-N thickness index surface index object plane surfaces image plane 2 3 j N-2 N-1 (N) 3... j... N-2 N-1 N
10 System data 10 Necessary data for system calculation: 1. system surfaces with parameters (radius) 2. distances with parameters (length, material) 3. stop surface 4. wavelength(s) 5. aperture 6. field point(s) Optional inputs: 1. finite diameters 2. vignetting factors 3. decenter and tilt 4. coordinate reference 5. weighting factors 6. multi configurations 7....
11 11 Definition of Aperture and Field Imaging on axis: circular / rotational symmetry Only spherical aberration and chromatical aberrations Finite field size, object point off-axis: - chief ray as reference y y p y' p y' - skew ray bundels: coma and distortion - Vignetting, cone of ray bundle not circular symmetric - to distinguish: tangential and sagittal plane O object plane marginal/rim ray u w entrance pupil chief ray chief ray exit pupil R' AP w' u' image plane O'
12 12 Aperture Definition Quantitative measures of relative opening / size of accepted light cone Numerical aperture NA n F-number sin u' exit pupil image plane F# f ' D EX chief ray Approximation for small apertures: D EX W' U' 1 F# 2 NA marginal ray f'
13 13 Important Test Wavelengths in [nm] Name Color Element UV Hg UV Hg UV Hg UV Hg UV Hg i UV Hg h violett Hg g blau Hg F' blau Cd F blau H e grün Hg d gelb He D gelb Na HeNe-Laser C' rot Cd C rot H r rot He s IR Cä t IR Hg Nd:YAG-Laser
14 14 Important Surface Types Standard Even asphere Paraxial Paraxial XY Coordinate break Diffraction grating Gradient 1 Toroidal Zernike Fringe sag Extended polynomial Black Box Lens ABCD spherical and conic sections classical asphere ideal lens ideal toric lens change of coordinate system line grating gradient medium cylindrical lens surface as superposition of Zernike functions generalized asphere hidden system, from vendors paraxial segment
15 Settings and Environment 15 The settings can be customized in the preferences All the settings can be saved Important: - data file folders - graphics parameters - editor cell size and Text font - preferred fast button functions - colors - language (don t use German!)
16 16 Zemax interface Helpful shortcuts: 1. F3 undo 2. F2 edit a cell in the editor 3. cntr A multiconfiguration toggle 4. cntr V variable toggle 5. F6 merit function editor 6. cntr U update 7. shift cntr Q quick focus Window options: 1. several export options 2. fixed aspect ratios 3. clone 4. adding comments or graphics
17 17 System data tables Menu: Menu: Reports / Prescription data reports / prescription data
18 System data tables 18
19 19 Selection of Wavelengths Setting of wavelengths: - maximum of 24 values - weighting factors allow for spectral modelling - unit is always mm - selection of primary wavelength: paraxial data are based on it
20 20 3D Geometry General input of tilt and decenter: Coordinate break surface Change of coordinate system with lateral translation and 3 rotations angles Direct listing in lens editor Not shown in layout drawing
21 21 3D Geometry Auxiliary menus: 1. Tilt/Decenter element 2. Folding mirror
22 22 3D Geometry Local tilt and decenter of a surface 1. no direct visibility in lens editor only + near surface index 2. input in surface properties 3. with effect on following system surfaces
23 23 Surface properties and settings Setting of surface properties surface type additional drawing switches diameter local tilt and decenter operator and sampling for POP coating scattering options
24 24 Important Surface Types Special surface types Data in Lens Data Editor or in Extra Data Editor Gradient media are descriped as 'special surfaces' Diffractive / micro structured surfaces described by simple ray tracing model in one order
Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term
Lens Design I Lecture 3: Properties of optical systems II 205-04-27 Herbert Gross Summer term 205 www.iap.uni-jena.de 2 Preliminary Schedule 3.04. Basics 2 20.04. Properties of optical systems I 3 27.05.
More informationLens Design I. Lecture 4: Properties of optical systems III Herbert Gross. Summer term
Lens Design I Lecture 4: Properties of optical systems III 018-05-03 Herbert Gross Summer term 018 www.iap.uni-jena.de Preliminary Schedule - Lens Design I 018 1 1.04. Basics 19.04. Properties of optical
More informationLens Design I. Lecture 2: Properties of optical systems I Herbert Gross. Summer term
Lens Design I Lecture 2: Properties of optical systems I 2015-04-20 Herbert Gross Summer term 2015 www.iap.uni-jena.de 2 Preliminary Schedule 1 13.04. Basics 2 20.04. Properties of optical systems I 3
More informationLens Design I. Lecture 2: Properties of optical systems I Herbert Gross. Summer term
Lens Design I Lecture 2: Properties of optical systems I 2018-04-19 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
More informationLens Design I. Lecture 11: Imaging Herbert Gross. Summer term
Lens Design I Lecture 11: Imaging 2015-06-29 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. 4 04.05. Properties
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 10: Advanced handling II 2014-06-20 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 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 informationOptical Design with Zemax
Optical Design with Zemax Lecture 2: Properties of optical systems I 2014-04-18 Herbert Gross Sommer term 2014 www.iap.uni-ena.de 2 Preliminary Schedule 1 11.04. Introduction 2 18.04. Properties of optical
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 7: Optimization I 2012-12-11 Herbert Gross Winter term 2012 www.iap.uni-jena.de Time schedule 2 1 16.10. Introduction Introduction, Zemax interface, menues, file handling,
More informationLens Design I. Lecture 9: OptimizationI Herbert Gross. Summer term
Lens Design I Lecture 9: OptimizationI 2015-06-15 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. 4 04.05. Properties
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 10: Advanced handling 2013-06-28 Herbert Gross Summer term 2013 www.iap.uni-jena.de 2 Preliminary Schedule 1 12.04. Introduction 2 19.04. Properties of optical systems
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 1: Introduction 2012-07-17 Herbert Gross Summer term 2012 www.iap.uni-ena.de Lecture data 2 Planned dates: 17.07. 24.07. 14.08. 28.08. 11.09. 25.09. 09.10. 23.10. 06.11.
More informationAdvanced Lens Design
Advanced Lens Design Lecture 3: Optimization II 2013-10-29 Herbert Gross Winter term 2013 www.iap.uni-jena.de 2 Preliminary Schedule 1 15.10. Introduction Paraxial optics, ideal lenses, optical systems,
More informationOptical Design with Zemax for PhD - Basics
Optical Design with Zemax for PhD - Basics Lecture 8: Advanced handling 2013-06-27 Herbert Gross Summer term 2013 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed content 1 02.05. Introduction
More informationOptical Design with Zemax
Optical Design with Zemax Lecture : Properties of optical sstems II 0-0-30 Herbert Gross Winter term 0 www.iap.uni-jena.de Properties of Optical Sstems II Preliminar time schedule 6.0. Introduction Introduction,
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 2: Properties of optical systems I 2012-10-23 Herbert Gross Winter term 2012 www.iap.uni-ena.de Preliminary time schedule 2 1 16.10. Introduction Introduction, Zemax interface,
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 3: Properties of optical sstems II 04-04-8 Herbert Gross Sommer term 04 www.iap.uni-jena.de Preliminar Schedule.04. Introduction 8.04. Properties of optical sstems I 3
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 9: Illumination 2013-06-14 Herbert Gross Summer term 2013 www.iap.uni-jena.de 2 Preliminary Schedule 1 12.04. Introduction 2 19.04. Properties of optical systems I 3 26.04.
More informationOptical Design with Zemax for PhD
Optical Design with Zemax for PhD Lecture 8: Advanced handling 2016-01-27 Herbert Gross Winter term 2015 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed content 1 11.11. Introduction
More informationOptical Design with Zemax for PhD
Optical Design with Zemax for PhD Lecture : Physical Optics 06-03-3 Herbert Gross Winter term 05 www.iap.uni-jena.de Preliminary Schedule No Date Subject Detailed content.. Introduction 0.. Basic Zemax
More informationFeature Map. Work the way you want, faster, easier... with the same Zemax reliability. RIBBONS / EDITORS
Feature Map Feature Map Work the way you want, faster, easier... with the same Zemax reliability. Zemax brings a new level of productivity to optics simulation software with OpticStudio14. Built on Zemax
More informationLens Design. Craig Olson. Julie Bentley. Field Guide to. John E. Greivenkamp, Series Editor SPIE. SPIE Field Guides. Volume FG27
Field Guide to Lens Design Julie Bentley Craig Olson SPIE Field Guides Volume FG27 John E. Greivenkamp, Series Editor SPIE PRESS Bellingham,Washington USA vii Glossary of Symbols and Acronyms xi Fundamentals
More informationOptical Design with Zemax for PhD
Optical Design with Zemax for PhD Lecture 6: Optimization I 2016-01-06 Herbert Gross Winter term 2015 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed content 1 11.11. Introduction 2
More informationAdvanced Lens Design
Advanced Lens Design Lecture 9: Field flattening 04--6 Herbert Gross Winter term 04 www.iap.uni-ena.de Preliminary Schedule.0. Basics Paraxial optics, imaging, Zemax handling 8.0. Optical systems Optical
More informationGeometrical Optics. Chapter General Comments. 1.2 Snell s Law
Chapter 1 Geometrical Optics 1.1 General Comments A light wave is an electromagnetic wave, and the wavelength that optics studies ranges from the ultraviolet (0.2 mm) to the middle infrared (10 mm). The
More informationTutorial Zemax 6: Advanced handling
Tutorial Zemax 6: Advanced handling 2012-09-25 6 Advanced handling 1 6.1 Multi configuration, universal plot and slider... 1 6.2 Macro for Spot Moments... 6 6.3 Multiconfiguration and folding mirror...
More informationRefraction at a single curved spherical surface
Refraction at a single curved spherical surface This is the beginning of a sequence of classes which will introduce simple and complex lens systems We will start with some terminology which will become
More informationEfficient wave-optical calculation of 'bad systems'
1 Efficient wave-optical calculation of 'bad systems' Norman G. Worku, 2 Prof. Herbert Gross 1,2 25.11.2016 (1) Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany (2)
More informationFundamental Optics for DVD Pickups. The theory of the geometrical aberration and diffraction limits are introduced for
Chapter Fundamental Optics for DVD Pickups.1 Introduction to basic optics The theory of the geometrical aberration and diffraction limits are introduced for estimating the focused laser beam spot of a
More information18.4 Release Notes May 10th, 2018
18.4 Release Notes May 10 th, 2018 CONTENTS 1 Sequential Features... 3 1.1 Full-Field Aberration analysis (Professional and Premium editions)... 3 1.2 GRIN surface usage with User-Defined and Grid Sag
More informationImaging and Aberration Theory
Imaging and Aberration Theory Lecture 8: Astigmastism and field curvature 03--9 Herbert Gross Winter term 03 www.iap.uni-jena.de Preliminary time schedule 4.0. Paraxial imaging paraxial optics, fundamental
More informationFinal Exam. Today s Review of Optics Polarization Reflection and transmission Linear and circular polarization Stokes parameters/jones calculus
Physics 42200 Waves & Oscillations Lecture 40 Review Spring 206 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 2 You can bring one double-sided pages of notes/formulas.
More informationWaves & Oscillations
Physics 42200 Waves & Oscillations Lecture 40 Review Spring 2016 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 112 You can bring one double-sided pages of notes/formulas.
More informationImaging and Aberration Theory
Imaging and Aberration Theory Lecture 8: Astigmatism and field curvature 0--4 Herbert Gross Winter term 0 www.iap.uni-jena.de Preliminary time schedule 9.0. Paraxial imaging paraxial optics, fundamental
More informationAdvanced Lens Design
Advanced Lens Design Lecture : Introduction 3--5 Herbert Gross Winter term 3 www.iap.uni-jena.de Overview Time: Tuesday, 8.5 9.45 Location: PaPool, Helmholtweg 4 Web page on IAP homepage under learning/materials
More informationWaves & Oscillations
Physics 42200 Waves & Oscillations Lecture 41 Review Spring 2013 Semester Matthew Jones Final Exam Date:Tuesday, April 30 th Time:1:00 to 3:00 pm Room: Phys 112 You can bring two double-sided pages of
More informationContrast Optimization: A faster and better technique for optimizing on MTF ABSTRACT Keywords: INTRODUCTION THEORY
Contrast Optimization: A faster and better technique for optimizing on MTF Ken Moore, Erin Elliott, Mark Nicholson, Chris Normanshire, Shawn Gay, Jade Aiona Zemax, LLC ABSTRACT Our new Contrast Optimization
More informationRay Tracing. Lens Design OPTI 517. Prof. Jose Sasian
Ray Tracing Lens Design OPTI 517 Use of rays In optical design In computer graphics In acoustics In art In photography Lens design ray-tracing Ray tracing universe Ray tracing It is important to have
More informationOptical Design with Zemax for PhD - Advanced
Optical Design with Zemax for PhD - Advanced Seminar 9 : Advanced Topics 2015-02-04 Herbert Gross Winter term 2014 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed content 1 12.11. Repetition
More informationDiffraction. Single-slit diffraction. Diffraction by a circular aperture. Chapter 38. In the forward direction, the intensity is maximal.
Diffraction Chapter 38 Huygens construction may be used to find the wave observed on the downstream side of an aperture of any shape. Diffraction The interference pattern encodes the shape as a Fourier
More informationDesign and Correction of optical Systems
Design and Correction of optical Systems Part 3: Components Summer term 0 Herbert Gross Overview. Basics 0-04-8. Materials 0-04-5 3. Components 0-05-0 4. Paraxial optics 0-05-09 5. Properties of optical
More informationOptical Design with Zemax for PhD
Optical Design with Zemax for PhD Lecture 3: Tolerancing I 26-4-8 Herbert Gross Winter term 25 / Summer term 26 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed content.. Introduction
More informationMedical Photonics Lecture 1.2 Optical Engineering
Medical Photonics Lecture 1.2 Optical Engineering Lecture 4: Components 2017-11-16 Michael Kempe Winter term 2017 www.iap.uni-jena.de 2 Contents No Subject Ref Detailed Content 1 Introduction Gross Materials,
More informationAberration Theory. Lens. Optical systems convert the shapes of wavefronts
Aberration Theory Lens Optical systems convert the shapes of wavefronts Aberrations A perfectly spherical wave will converge to a point. Any deviation from the ideal spherical shape is said to be an aberration.
More informationSection 10. Stops and Pupils
10-1 Section 10 Stops and Pupils Stops and Pupils The aperture stop is the aperture in the system that limits the bundle of light that propagates through the system from the axial object point. The stop
More informationFRED Slit Diffraction Application Note
FRED Slit Diffraction Application Note The classic problem of diffraction through a slit finds one of its chief applications in spectrometers. The wave nature of these phenomena can be modeled quite accurately
More informationAP Physics: Curved Mirrors and Lenses
The Ray Model of Light Light often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization, but is very useful for geometric
More informationGiven are two refracting media separated by a spherical surface. From the point O an arbitrary ray OM is emitted (Fig 1). This ray is refracted at
This lecture is based on a Leon Magiera s paper and on a very extended exchange of emails between him and the presenter who produced the final presentation assisted by many comments of Leon. All graphics
More informationLight: Geometric Optics (Chapter 23)
Light: Geometric Optics (Chapter 23) Units of Chapter 23 The Ray Model of Light Reflection; Image Formed by a Plane Mirror Formation of Images by Spherical Index of Refraction Refraction: Snell s Law 1
More informationAberrations in Holography
Aberrations in Holography D Padiyar, J Padiyar 1070 Commerce St suite A, San Marcos, CA 92078 dinesh@triple-take.com joy@triple-take.com Abstract. The Seidel aberrations are described as they apply to
More informationGeometric Optics. The Law of Reflection. Physics Waves & Oscillations 3/20/2016. Spring 2016 Semester Matthew Jones
Physics 42200 Waves & Oscillations Lecture 27 Propagation of Light Hecht, chapter 5 Spring 2016 Semester Matthew Jones Geometric Optics Typical problems in geometric optics: Given an optical system, what
More informationMetrology and Sensing
Metrology and Sensing Lecture 11: Measurement of basic system properties 017-01-03 Herbert Gross Winter term 016 www.iap.uni-jena.de Preliminary Schedule No Date Subject Detailed Content 1 18.10. Introduction
More informationLens Design II. Lecture 12: Mirror systems Herbert Gross. Winter term
Lens Design II Lecture 1: Mirror systems 017-01-11 Herbert Gross Winter term 016 www.iap.uni-jena.de Preliminary Schedule 1 19.10. Aberrations and optimization Repetition 6.10. Structural modifications
More informationChapter 36. Image Formation
Chapter 36 Image Formation Apr 22, 2012 Light from distant things We learn about a distant thing from the light it generates or redirects. The lenses in our eyes create images of objects our brains can
More informationOPTI 513R / Optical Testing
OPTI 513R / Optical Testing Instructor: Dae Wook Kim Meinel Building Rm 633, University of Arizona, Tucson, AZ 85721 E-Mail: dkim@optics.arizona.edu Website: sites.google.com/site/opti513r/ Office Hours:
More informationChapter 3 Geometric Optics
Chapter 3 Geometric Optics [Reading assignment: Goodman, Fourier Optics, Appendix B Ray Optics The full three dimensional wave equation is: (3.) One solution is E E o ûe i ωt± k r ( ). This is a plane
More informationParaxial into real surfaces
Paraxial into real surfaces Curvature, Radius Power lens and mirrors lens maker equation mirror and lens in contact Principle planes Real Surfaces Refractive via Fermat s Principle Calculate optical path
More informationEE119 Homework 3. Due Monday, February 16, 2009
EE9 Homework 3 Professor: Jeff Bokor GSI: Julia Zaks Due Monday, February 6, 2009. In class we have discussed that the behavior of an optical system changes when immersed in a liquid. Show that the longitudinal
More informationBasic optics. Geometrical optics and images Interference Diffraction Diffraction integral. we use simple models that say a lot! more rigorous approach
Basic optics Geometrical optics and images Interference Diffraction Diffraction integral we use simple models that say a lot! more rigorous approach Basic optics Geometrical optics and images Interference
More informationINFINITY-CORRECTED TUBE LENSES
INFINITY-CORRECTED TUBE LENSES For use with Infinity-Corrected Objectives Available in Focal Lengths Used by Thorlabs, Nikon, Leica, Olympus, and Zeiss Designs for Widefield and Laser Scanning Applications
More informationGetting Started Using ZEMAX
Getting Started Using ZEMAX Version 2.1 Table of Contents 1 ABOUT THIS GUIDE... 3 2 INSTALLING ZEMAX... 4 2.1 INSTALLING THE KEY DRIVER... 4 2.2 INSTALLING RZ PREREQUISITES... 4 2.3 INSTALLING ZEMAX...
More informationOptics and Images. Lenses and Mirrors. Matthew W. Milligan
Optics and Images Lenses and Mirrors Light: Interference and Optics I. Light as a Wave - wave basics review - electromagnetic radiation II. Diffraction and Interference - diffraction, Huygen s principle
More informationMeet Your Augmented and Virtual Reality Challenges Head-On: Design Your Next System with 2D-Q Freeforms in CODE V
WHITE PAPER Meet Your Augmented and Virtual Reality Challenges Head-On: Design Your Next System with 2D-Q Freeforms in CODE V Author Matt Novak, Ph.D. CODE V Sr. Customer Applications Engineer, Synopsys
More informationPhys102 Lecture 21/22 Light: Reflection and Refraction
Phys102 Lecture 21/22 Light: Reflection and Refraction Key Points The Ray Model of Light Reflection and Mirrors Refraction, Snell s Law Total internal Reflection References 23-1,2,3,4,5,6. The Ray Model
More informationAlgebra Based Physics
Slide 1 / 66 Slide 2 / 66 Algebra Based Physics Geometric Optics 2015-12-01 www.njctl.org Table of ontents Slide 3 / 66 lick on the topic to go to that section Reflection Spherical Mirror Refraction and
More informationOPTI-502 Optical Design and Instrumentation I John E. Greivenkamp Final Exam In Class Page 1/12 Fall, 2017
Final Exam In Class Page / Fall, 07 Name SOLUTIONS Closed book; closed notes. Time limit: 0 minutes. An equation sheet is attached and can be removed. Spare raytrace sheets are attached. Use the back sides
More informationLIGHT. Speed of light Law of Reflection Refraction Snell s Law Mirrors Lenses
LIGHT Speed of light Law of Reflection Refraction Snell s Law Mirrors Lenses Light = Electromagnetic Wave Requires No Medium to Travel Oscillating Electric and Magnetic Field Travel at the speed of light
More informationRay Optics I. Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex
Phys 531 Lecture 8 20 September 2005 Ray Optics I Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex Today shift gears, start applying
More informationFormulas of possible interest
Name: PHYS 3410/6750: Modern Optics Final Exam Thursday 15 December 2011 Prof. Bolton No books, calculators, notes, etc. Formulas of possible interest I = ɛ 0 c E 2 T = 1 2 ɛ 0cE 2 0 E γ = hν γ n = c/v
More informationLight: Geometric Optics
Light: Geometric Optics 23.1 The Ray Model of Light Light very often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization,
More informationPart Images Formed by Flat Mirrors. This Chapter. Phys. 281B Geometric Optics. Chapter 2 : Image Formation. Chapter 2: Image Formation
Phys. 281B Geometric Optics This Chapter 3 Physics Department Yarmouk University 21163 Irbid Jordan 1- Images Formed by Flat Mirrors 2- Images Formed by Spherical Mirrors 3- Images Formed by Refraction
More informationPhysics 123 Optics Review
Physics 123 Optics Review I. Definitions & Facts concave converging convex diverging real image virtual image real object virtual object upright inverted dispersion nearsighted, farsighted near point,
More informationTolerance on material inhomogenity and surface irregularity
Opti 521 Wenrui Cai Tolerance on material inhomogenity and surface irregularity Abstract In this tutorial, a case study on tolerance for a focusing doublet is performed by using ZEMAX. First, how to perform
More informationLight & Optical Systems Reflection & Refraction. Notes
Light & Optical Systems Reflection & Refraction Notes What is light? Light is electromagnetic radiation Ultra-violet + visible + infra-red Behavior of Light Light behaves in 2 ways particles (photons)
More informationOptical design of COrE+
Optical design of COrE+ Karl Young November 23, 2015 The optical designs for COrE+ were made by Darragh McCarthy and Neil Trappe at Maynooth University and Karl Young and Shaul Hanany at University of
More informationApplication-Specific Optical Design
Application-Specific Optical Design Introduction Optical design software capabilities have advanced considerably from the late 1950s and early 1960s when computer tools first became available. Initially,
More informationRefractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different
Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different types of lens systems used Want to look at each from
More informationRay Optics Demonstration Set (RODS) and Ray Optics Demonstration Set Plus (RODS+) USER S GUIDE
Ray Optics Demonstration Set (RODS) and Ray Optics Demonstration Set Plus USER S GUIDE 1 NO. OF EXP. Table of contents TITLE OF EXPERIMENT SET TO USE Introduction Tables of the set elements E1 Reflection
More informationContents. Ray Intersection Patterns Spherical Coma Field Curvature and astigmatism Distortion Aplanatic Points How to reduce aberrations
Contents Ray Intersection Patterns Spherical Coma Field Curvature and astigmatism Distortion Aplanatic Points How to reduce aberrations ECE 4616 Tolis Deslis Contents Contents Ray Intersection Patterns
More information3B SCIENTIFIC PHYSICS
3B SCIENTIFIC PHYSICS Instruction sheet 06/18 ALF Laser Optics Demonstration Set Laser Optics Supplement Set Page 1 2 3 3 3 4 4 4 5 5 5 6 6 6 7 7 7 8 8 8 9 9 9 10 10 10 11 11 11 12 12 12 13 13 13 14 14
More informationPH880 Topics in Physics
PH880 Topics in Physics Modern Optical Imaging (Fall 2010) The minimum path principle n(x,y,z) Γ Γ has the minimum optical path length, compared to the alternative paths. nxyzdl (,, ) Γ Thelaw of reflection
More informationUsing Skew Rays to Model Gaussian Beams
Using Skew Rays to Model Gaussian Beams Host: Paul Colbourne, Lumentum Zemax, LLC 2016 1 Topics we ll cover today: Using skew rays to represent a Gaussian beam. Use of User-Defined Surfaces to generate
More informationMedical Photonics Lecture Optical Engineering
Medical Photonics Lecture Optical Engineering Lecture 13: Metrology 2018-02-01 Herbert Gross Winter term 2017 www.iap.uni-jena.de 2 Schedule Optical Engineering 2017 No Subject Ref Date Detailed Content
More informationRefractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different
Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different types of lens systems used Want to look at each from
More informationHistory of Light. 5 th Century B.C.
History of Light 5 th Century B.C. Philosophers thought light was made up of streamers emitted by the eye making contact with an object Others thought that light was made of particles that traveled from
More informationTEAMS National Competition High School Version Photometry 25 Questions
TEAMS National Competition High School Version Photometry 25 Questions Page 1 of 14 Telescopes and their Lenses Although telescopes provide us with the extraordinary power to see objects miles away, the
More informationPractical Use of Saddle-Point Construction in Lens Design
Practical Use of Saddle-Point Construction in Lens Design Zhe Hou a, Irina Livshits b, and Florian Bociort a a Optics Research Group, Delft University of Technology, Lorentzweg 1, 2628CJ Delft, The Netherlands;
More informationSection 2. Mirror and Prism Systems
2-1 Section 2 Mirror and Prism Systems Plane Mirrors Plane mirrors are used to: Produce a deviation Fold the optical path Change the image parity Each ray from the object point obeys the law of reflection
More informationindex of refraction-light speed
AP Physics Study Guide Chapters 22, 23, 24 Reflection, Refraction and Interference Name Write each of the equations specified below, include units for all quantities. Law of Reflection Lens-Mirror Equation
More informationContrast Optimization A new way to optimize performance Kenneth Moore, Technical Fellow
Contrast Optimization A new way to optimize performance Kenneth Moore, Technical Fellow What is Contrast Optimization? Contrast Optimization (CO) is a new technique for improving performance of imaging
More informationLecture Outline Chapter 26. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.
Lecture Outline Chapter 26 Physics, 4 th Edition James S. Walker Chapter 26 Geometrical Optics Units of Chapter 26 The Reflection of Light Forming Images with a Plane Mirror Spherical Mirrors Ray Tracing
More informationExercise 12 Geometrical and Technical Optics WS 2013/2014
Exercise 12 Geometrical and Technical Optics WS 213/214 Slide projector and Köhler illumination In this exercise a simplified slide projector (or LCD projector) will be designed and simulated with ray
More informationLIGHT & OPTICS. Fundamentals of Physics 2112 Chapter 34 1
LIGHT & OPTICS Fundamentals of Physics 22 Chapter 34 Chapter 34 Images. Two Types of Images 2. Plane Mirrors 3. Spherical Mirrors 4. Images from Spherical Mirrors 5. Spherical Refracting Surfaces 6. Thin
More informationRefractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different
Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different types of lens systems used Want to look at each from
More informationIntroduction. Past Homework solutions Optimization Test Plate fitting Tolerance routine Homework. ECE 4616 Deslis
Introduction Past Homework solutions Optimization Test Plate fitting Tolerance routine Homework 1 Optimization Optimization is one of the most important features in Zemax. We use optimization to be able
More informationChapter 7: Geometrical Optics. The branch of physics which studies the properties of light using the ray model of light.
Chapter 7: Geometrical Optics The branch of physics which studies the properties of light using the ray model of light. Overview Geometrical Optics Spherical Mirror Refraction Thin Lens f u v r and f 2
More informationLight: Geometric Optics
Light: Geometric Optics The Ray Model of Light Light very often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization, but
More informationOptics Course (Phys 311) Geometrical Optics Refraction through Lenses
Optics Course (Phys ) Geometrical Optics Refraction through Lenses Lecturer: Dr Zeina Hashim Slide 1 Objectives covered in this lesson : 1. Refraction through single spherical refracting surfaces. 2. Lenses:
More informationChapter 33 Continued Properties of Light. Law of Reflection Law of Refraction or Snell s Law Chromatic Dispersion Brewsters Angle
Chapter 33 Continued Properties of Light Law of Reflection Law of Refraction or Snell s Law Chromatic Dispersion Brewsters Angle Dispersion: Different wavelengths have different velocities and therefore
More informationLecture 4 Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization
Lecture 4 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,
More information