Tolerancing in CODE V
|
|
- Kerry Hoover
- 6 years ago
- Views:
Transcription
1 Tolerancing in CODE V 3280 East Foothill Boulevard Pasadena, California USA (626) Fax (626) service@opticalres.com World Wide Web:
2 About This Presentation This presentation consists of: A PowerPoint show to introduce and describe CODE V s tolerancing features A few demonstrations to show how the features work in CODE V Tolerancing in CODE V, Slide-2
3 What is Tolerancing? Tolerancing is complex interactive process required for any system that will be fabricated, steps include: Definition of fabrication and assembly tolerance budget Definition of fabrication and alignment compensators, and an alignment plan Success requires the ability to accurately predict individual tolerance sensitivities & the as-built performance of the entire system, including the effects of compensation Tolerancing in CODE V, Slide-3
4 What Does Tolerancing Tells Us? Which lens parameters are the most sensitive to manufacture or align Which compensator or compensators are effective for assembly or alignment What is the probability of achieving a given performance level for the fabricated system Cumulative Probability (%) Cooke Triplet f/4.5 Tolerance Analysis ORA Jun-02 Field 1 Field 2 Field 3 80% probability of achieving ~0.88 MTF for Field 1 -or- 80% of built systems will have about 0.88 MTF or better at Field Modulation Transfer Function Typical Cumulative Probability Curve Tolerancing in CODE V, Slide-4
5 Why is Tolerancing Important? Cost reduction! When attacked with the right tools, tolerancing can significantly reduce: Non-recurring costs including designer time, production tool development, and definition of assembly/alignment procedures Recurring costs including system fabrication, assembly, and alignment The design that meets spec with the loosest tolerances and the best compensator set will minimize manufacturing and assembly costs! Tolerancing in CODE V, Slide-5
6 CODE V s Tolerancing Options Analysis > Tolerancing menu allows you to choose among CODE V s various methods for computing the performance impact of manufacturing and assembly errors CODE V s primary tolerancing option, TOR, supports the following performance metrics Diffraction MTF RMS wavefront error Fiber Coupling Efficiency Polarization Dependent Loss Zernike Wavefront Coefficients (command line only) Tolerancing in CODE V, Slide-6
7 How TOR works TOR uses a fast wavefront differential algorithm to determine the performance impact due to tolerances Required information computed from a real ray trace of the nominal system Includes cross-terms, the impact of interacting tolerances TOR can be 50x to 1000x faster than alternative tolerancing methods This allows TOR to be use early and frequently during the design process Tolerancing in CODE V, Slide-7
8 TOR Modes of Operation Inverse mode - computes the tolerance values so each tolerance has approximately the same impact on performance (default mode) However, tolerances will never violate userdefined minimum & maximum limits Individual tolerance values can be frozen to not change during an Inverse mode analysis if desired Sensitivity mode - computes the effects of specified tolerances on performance CODE V will not try to change the tolerance values Tolerancing in CODE V, Slide-8
9 2-Parameter TOR Demonstration Tolerancing in CODE V, Slide-9
10 What Does This Example Show Us? TOR is easy to use For real systems, compensation is crucial Realistic tolerance limits can be imposed TOR s inverse sensitivity analysis will help reduce system sensitivity by attempting to set each tolerance to contribute equally to the performance degradation of the system Tolerancing in CODE V, Slide-10
11 Assumptions of the Wavefront Differential method Only applicable to a subset of performance metrics that can be adequately described by an exit pupil function Fundamental assumption is that optical path differences induced by tolerance perturbations for each ray in the ray grid vary linearly with tolerance change Valid when tolerance change results in a small degradation of the nominal performance (typically true for tolerances) Wavefront differential equations requires knowledge of how each tolerance affects the system This means that only CODE V pre-programmed tolerance types can be analyzed Tolerancing in CODE V, Slide-11
12 Entry of Tolerances Along with the Surface Properties window you can also use Review > Tolerances Enter specific tolerances using drop-down menu Tolerancing in CODE V, Slide-12
13 Default Tolerances Default tolerances can be generated for a surface or range of surfaces via the Autofill button on the Tolerance Review Tolerancing in CODE V, Slide-13
14 CODE V Tolerance Types Tolerances on single surfaces Radius, thickness, index, etc. Tolerances on elements Wedge Tolerances on components (single elements or cemented elements) Decenter, tilt, etc. Tolerances on polarization properties Retardance, Faraday rotation, etc. CODE V tolerances are used by TOR and a large subset are used by other tolerancing features Tolerancing in CODE V, Slide-14
15 Single Surface Tolerances: Radius Changes in radius DLR (delta radius) DLC (delta curvature) DLS (delta sag at clear aperture) DLF (delta fringe - test plate fit) DLF S2 IRR (cylindrical irregularity in fringes) CYN (cylinder normal - oriented at 0 ) CYD (cylinder diagonal - oriented at 45 ) irregularity Underlined tolerances indicate Default tolerance types Photo of actual test plate fit Tolerancing in CODE V, Slide-15
16 Single Surface Tolerances: Sag Change in surface sag in waves at the fringe wavelength, defined by Standard or Fringe Zernike coefficients (can be applied to any surface type) ZRN Cm (Standard Zernike coefficient) ZFR Cm (Fringe Zernike coefficient) Tolerancing in CODE V, Slide-16
17 Single Surface Tolerances: Index, Thickness Changes in refractive index DLN (delta index) DLV (delta V value) Only used if there are three wavelengths or more HOM (homogeneity) AXG (axial index gradient) RAG (radial quadratic index gradient) DLT (change in thickness) DLT S1 Tolerancing in CODE V, Slide-17
18 Single Surface Tolerances: Shape Change in aspheric coefficients (can be applied to any surface type) DAK (delta conic constant) DAA (delta A - 4th order coefficient) DAB (delta B - 6th order coefficient) DAC (delta C - 8th order coefficient) DAD (delta D -10th order coefficient) DAE (delta E - 12th order coefficient) DAF (delta F - 14th order coefficient) DAG (delta G - 16th order coefficient) DAH (delta H - 18th order coefficient) DAJ (delta J - 20th order coefficient) Cosine ripple and random surface error RPA, RPS (cosine ripple amplitude and slope) RSE (random surface error) Tolerancing in CODE V, Slide-18
19 Single Surface Decenter and Displacement Tolerances Decentration tolerances DEC (decenter) DLX (delta shift in X) DLY (delta shift in Y) DLZ (delta shift in Z) Tilt tolerances TIL (tilt) DLA (delta tilt in alpha in radians) DLB (delta tilt in beta in radians) DLG (delta tilt in gamma in radians) Wedge tolerances TIR (total indicated reading) TRX (TIR in X) TRY (TIR in Y) DLY S1 A DLA S1 TIR S1 = A - B B Tolerancing in CODE V, Slide-19
20 Group Decenter and Displacement Tolerances Group tilt BTI (barrel tilt in radians) BTX (barrel tilt in X in radians) BTY (barrel tilt in Y in radians) BRL (barrel roll about Z in radians) Group displacement DIS (displacement) DSX (displacement in X) DSY (displacement in Y) DSZ (displacement in Z) Group roll (cemented surfaces) ROL (roll) RLX (roll in X) RLY (roll in Y) R = reverse (roll about second surface) DSY S1..2 BTY S1..2 RLY S1..2 R Tolerancing in CODE V, Slide-20
21 Group Tolerances (cont.) DOL (delta overall length - change is divided among each surface) STI (shear tolerance - each surface is independently tilted) STX (shear in X) STY (shear in Y) STY S1..2 Tolerancing in CODE V, Slide-21
22 Polarization Tolerances BMA, BMB, BMG Tolerance on tilt about X, Y, and Z crystal axes, respectively, for birefringent material BMN Tolerance on ordinary and extraordinary refractive index difference for birefringent materials PPA Amplitude transmittance tolerance for a leaky linear polarizer PPF Rotation angle tolerance for Faraday rotator PPR Retardance tolerance for ideal retarder PPO Rotation angle tolerance for polarizing elements Tolerancing in CODE V, Slide-22
23 Typical Tolerancing Example Define tolerances and compensator(s) Or use the CODE V default values Determine the tolerance performance metric of interest Enter required information (e.g., MTF spatial frequency and azimuth values) Modify tolerance limits Or use CODE V default limits Run TOR in inverse sensitivity mode Review results, optionally modify tolerance and compensator set, adjust performance change value, etc. & re-run TOR Tolerancing in CODE V, Slide-23
24 Demonstration - Typical TOR Run Tolerancing in CODE V, Slide-24
25 Wavefront Differential Tolerancing Statistics MTF MTF probability distribution MTF = A ΔP 2 + B ΔP + C σ Probability Nominal MTF (C) 50% change Nominal MTF MTF Nominal parameter value ΔP Impact of single compensated tolerance on MTF at one field "Probable change" Integral of 50% of cases Integral of 84% of cases (1σ) Integral of 98% of cases (2σ) Integral of 99.7% of cases (3σ) MTF performance probability distribution due to all tolerances (and compensation) at one field Tolerancing in CODE V, Slide-25
26 Interactive Tolerancing Interactive Tolerancing is a special spreadsheet interface that leverages the speed of TOR s wavefront differential algorithm Users can interactively change tolerance values and immediately see the impact on performance and compensator motion Tolerances causing the largest performance degradation are automatically put at the top of the list by default Tolerancing in CODE V, Slide-26
27 Interactive Tolerancing - Demonstration Tolerancing in CODE V, Slide-27
28 Other TOR Features Modeling your Optomechanical System accurately for TOR Coupled (Grouped) Tolerances Labeled Tolerances & Compensators Zoomed Tolerances & Compensators Tolerance X, Y, Z offsets TOR Compensation Solution using Singular Value Decomposition TOR Compensation for Magnification and Line-of- Sight Errors TOR Distortion Analysis Tolerancing in CODE V, Slide-28
29 Other Tolerancing Options Analysis > Tolerancing > Distortion Tolerancing for the performance metric of chief ray distortion (TOD) Also uses the fast wavefront differential algorithm Used when distortion or image mapping is the primary performance metric of interest Tolerancing in CODE V, Slide-29
30 Distortion Tolerancing (TOD) Two modes: Listing of change in chief ray locations with tolerances Difference between chief ray positions for two zoom positions Useful for biocular (i.e., two-eye) systems analysis Single zoom chief ray positional changes in X and Y with tolerances Tolerancing in CODE V, Slide-30
31 Other Tolerancing Options (cont.) User - Finite Differences Macro for finite-difference tolerancing using userdefined performance measures with optional userdefined tolerances (TOLFDIF) Useful for determining tolerance drivers, but performance summary does not include cross-terms User - Monte Carlo Macro for Monte Carlo tolerance analysis to simulate production yield using user-defined performance measures with optional user-defined tolerances (TOLMONTE) Useful for predicting system performance but includes no information about performance drivers Tolerancing in CODE V, Slide-31
32 What is Finite Differences Tolerancing? Each parameter is individually varied at the plus & minus limits of its tolerance range, compensation is typically achieved using optimization, and the system performance degradation is predicted on a tolerance-bytolerance basis These individual results are statistically combined to yield a total system performance prediction Tolerancing in CODE V, Slide-32
33 Pros & Cons of Finite Differences Tolerancing +Predicted performance sensitivity for individual tolerances is usually accurate, especially for tolerances that cause a large decrease in performance +Allows determination of performance drivers - Does not include cross-terms (i.e., how multiple tolerances interact), so overall performance prediction is generally optimistic - Accuracy of tolerance sensitivity prediction can be poor for tolerances that cause small performance changes - System must be analyzed (e.g., ray traced) twice for each tolerance (Typical triplet requires 100 ray traces) Tolerancing in CODE V, Slide-33
34 What is Monte Carlo Tolerancing? Simultaneously vary all of the parameters that have an associated tolerance randomly within each tolerance range, with compensation typically achieved using optimization The resulting system performance is analyzed This process is repeated many times with different random perturbations and results are statistically combined to yield a total system performance prediction Each analysis is called a trial Tolerancing in CODE V, Slide-34
35 Pros & Cons of Monte Carlo Tolerancing +Includes cross-terms (the impact of interacting tolerances), so system performance prediction can be accurate - No information about individual tolerance sensitivities - Requires one analysis (e.g., ray trace) per trial - Accurate predictions generally require 100 to 1000 trials! Tolerancing in CODE V, Slide-35
36 User Tolerancing - Demonstration Tolerancing in CODE V, Slide-36
37 Review: Pros of TOR +Provides information about individual tolerance sensitivities Like Finite Differences tolerancing +Provides accurate performance prediction since cross-terms are included Like Monte Carlo tolerancing +Method requires only a single analysis (ray trace) of the nominal system Can be 50x to 1000x faster than Finite Differences or Monte Carlo The speed of the wavefront differential algorithm allows tolerancing to become part of the design process, not just an end-of-the-project analysis Tolerancing in CODE V, Slide-37
38 Summary Tolerancing is a critical step in the optical design of systems that will be built CODE V s wavefront differential tolerancing feature, TOR, is fast and accurate Allows tolerancing to be done early and often during the design process CODE V s finite difference and Monte Carlo based tolerancing are available for performance metrics not handled by TOR Tolerancing in CODE V, Slide-38
CODE V Tolerancing: A Key to Product Cost Reduction
CODE V Tolerancing: A Key to Product Cost Reduction A critical step in the design of an optical system destined to be manufactured is to define a fabrication and assembly tolerance budget and to accurately
More informationTolerancing in Zemax. Lecture 4
Tolerancing in Zemax Lecture 4 Objectives: Lecture 4 At the end of this lecture you should: 1. Understand the reason for tolerancing and its relation to typical manufacturing errors 2. Be able to perform
More informationTolerancing in Zemax
Tolerancing in Zemax Rachel Haynes Opti 521 Tutorial December 10, 2007 Introduction Being able to design a good optical system is important as an optical engineer, but equally as important is being able
More informationCHAPTER 36 TOLERANCING TECHNIQUES
CHAPTER 36 TOLERANCING TECHNIQUES Robert R. Shannon Optical Sciences Center Uni ersity of Arizona Tucson, Arizona 3 6. 1 GLOSSARY a relative tolerance error BK7, SF2 types of optical glass C to F spectral
More information2. ADVANCED SENSITIVITY
Use of advanced sensitivity approach to novel optical compensation methods Mark C. Sanson & Keith Hanford Corning Incorporated, 60 O Connor Rd., Fairport, NY, USA 14450 ABSTRACT Understanding the sensitivity
More informationPractical Guide to Specifying Optical Components
Practical Guide to Specifying Optical Components OPTI 521 Introduction to Opto-Mechanical Engineering Fall 2012 December 10, 2012 Brian Parris Introduction This paper is intended to serve as a practical
More information12.4 Alignment and Manufacturing Tolerances for Segmented Telescopes
330 Chapter 12 12.4 Alignment and Manufacturing Tolerances for Segmented Telescopes Similar to the JWST, the next-generation large-aperture space telescope for optical and UV astronomy has a segmented
More informationSection 5 ISO Drawings ISO 10110
Section 5 ISO 10110 Drawings Optical Drawings provide a precise Definition of your optic for fabrication. Standards allow for a common language to be used between you and the optician so there is no confusion
More informationOctober 7, Peter Cheimets Smithsonian Astrophysical Observatory 60 Garden Street, MS 5 Cambridge, MA Dear Peter:
October 7, 1997 Peter Cheimets Smithsonian Astrophysical Observatory 60 Garden Street, MS 5 Cambridge, MA 02138 Dear Peter: This is the report on all of the HIREX analysis done to date, with corrections
More informationPROCEEDINGS OF SPIE. Measurement of low-order aberrations with an autostigmatic microscope
PROCEEDINGS OF SPIE SPIEDigitalLibrary.org/conference-proceedings-of-spie Measurement of low-order aberrations with an autostigmatic microscope William P. Kuhn Measurement of low-order aberrations with
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 informationOptical Engineering 421/521 Sample Questions for Midterm 1
Optical Engineering 421/521 Sample Questions for Midterm 1 Short answer 1.) Sketch a pechan prism. Name a possible application of this prism., write the mirror matrix for this prism (or any other common
More informationAn introduction to the new features in OSLO 6.5 and OSLO tolerancing
An introduction to the new features in OSLO 6.5 and OSLO tolerancing Presented by : Lambda Research Corporation 25 Porter Rd. Littleton, MA 01460 www.lambdares.com Presenter Steve Eckhardt President Eckhardt
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 informationTypical requirements of passive mm-wave imaging systems, and consequences for antenna design
Typical requirements of passive mm-wave imaging systems, and consequences for antenna design Rupert Anderton A presentation to: 6th Millimetre-wave Users Group NPL, Teddington 5 October 2009 1 1 Characteristics
More informationTolerancing. 280 Tolerancing. User-defined tolerancing
280 Tolerancing Tolerancing User-defined tolerancing User-defined tolerancing is a term used in OSLO to describe the process of settting tolerances when optical performance is measured by a user-defined
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 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 informationSystem Architecting: Defining Optical and Mechanical Tolerances from an Error Budget
System Architecting: Defining Optical and Mechanical Tolerances from an Error Budget Julia Zugby OPTI-521: Introductory Optomechanical Engineering, Fall 2016 Overview This tutorial provides a general overview
More informationRadial Polarization Converter With LC Driver USER MANUAL
ARCoptix Radial Polarization Converter With LC Driver USER MANUAL Arcoptix S.A Ch. Trois-portes 18 2000 Neuchâtel Switzerland Mail: info@arcoptix.com Tel: ++41 32 731 04 66 Principle of the radial polarization
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 informationPractical Plastic Optics
Practical Plastic Optics Practical Optics Seminar September 6, 2006 Mike Schaub Raytheon Missile Systems 1151 E. Hermans Road Tucson, AZ 85706 (520) 794-8162 Michael_P_Schaub@raytheon.com 1 Overview Plastic
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 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 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 informationTolerance analysis of lenses with high zoom ratio
Tolerance analysis of lenses with high zoom ratio Chir-Weei Chang, a, Gung-Hsuan Ho a, Chy-Lin Wang a, Wei-Chung Chao a, John D. Griffith b a Opto-Electronics & Systems Laboratories/Industrial Technology
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 informationFabrication of 6.5 m f/1.25 Mirrors for the MMT and Magellan Telescopes
Fabrication of 6.5 m f/1.25 Mirrors for the MMT and Magellan Telescopes H. M. Martin, R. G. Allen, J. H. Burge, L. R. Dettmann, D. A. Ketelsen, W. C. Kittrell, S. M. Miller and S. C. West Steward Observatory,
More informationUnderstanding Optical Specifications
Understanding Optical Specifications Optics can be found virtually everywhere, from fiber optic couplings to machine vision imaging devices to cutting-edge biometric iris identification systems. Despite
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 informationUNIT-II : SIGNAL DEGRADATION IN OPTICAL FIBERS
UNIT-II : SIGNAL DEGRADATION IN OPTICAL FIBERS The Signal Transmitting through the fiber is degraded by two mechanisms. i) Attenuation ii) Dispersion Both are important to determine the transmission characteristics
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 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 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 information3.0 Alignment Equipment and Diagnostic Tools:
3.0 Alignment Equipment and Diagnostic Tools: Alignment equipment The alignment telescope and its use The laser autostigmatic cube (LACI) interferometer A pin -- and how to find the center of curvature
More informationTechnical Report Synopsis: Chapter 4: Mounting Individual Lenses Opto-Mechanical System Design Paul R. Yoder, Jr.
Technical Report Synopsis: Chapter 4: Mounting Individual Lenses Opto-Mechanical System Design Paul R. Yoder, Jr. Introduction Chapter 4 of Opto-Mechanical Systems Design by Paul R. Yoder, Jr. is an introduction
More informationJ. C. Wyant Fall, 2012 Optics Optical Testing and Testing Instrumentation
J. C. Wyant Fall, 2012 Optics 513 - Optical Testing and Testing Instrumentation Introduction 1. Measurement of Paraxial Properties of Optical Systems 1.1 Thin Lenses 1.1.1 Measurements Based on Image Equation
More informationEUV projection optics and active mirror development at SAGEM
EUV projection optics and active mirror development at SAGEM R. Geyl,, M. Boutonne,, J.L. Carel,, J.F. Tanné, C. Voccia,, S. Chaillot,, J. Billet, Y. Poulard, X. Bozec SAGEM, Etablissement de St Pierre
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 informationTolerancing Primer. Marshall R. Scott. University of Arizona. December 17, 2015
Tolerancing Primer Marshall R. Scott University of Arizona marshallscott@email.arizona.edu December 17, 2015 1 Introduction The goal of the engineer is to design a system that meets a set of requirements
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 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 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 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 informationConformal optical system design with a single fixed conic corrector
Conformal optical system design with a single fixed conic corrector Song Da-Lin( ), Chang Jun( ), Wang Qing-Feng( ), He Wu-Bin( ), and Cao Jiao( ) School of Optoelectronics, Beijing Institute of Technology,
More informationUser s Guide Modulator Alignment Procedure
User s Guide Modulator Alignment Procedure Models 350, 360, 370, 380, 390 series Warranty Information ConOptics, Inc. guarantees its products to be free of defects in materials and workmanship for one
More informationCODE V Introductory Tutorial
CODE V Introductory Tutorial Cheng-Fang Ho Lab.of RF-MW Photonics, Department of Physics, National Cheng-Kung University, Tainan, Taiwan 1-1 Tutorial Outline Introduction to CODE V Optical Design Process
More informationRefractive index homogeneity TWE effect on large aperture optical systems
Refractive index homogeneity TWE effect on large aperture optical systems M. Stout*, B. Neff II-VI Optical Systems 36570 Briggs Road., Murrieta, CA 92563 ABSTRACT Sapphire windows are routinely being used
More informationThe Design, Fabrication, and Application of Diamond Machined Null Lenses for Testing Generalized Aspheric Surfaces
The Design, Fabrication, and Application of Diamond Machined Null Lenses for Testing Generalized Aspheric Surfaces James T. McCann OFC - Diamond Turning Division 69T Island Street, Keene New Hampshire
More informationLithography SMASH Sensor Objective Design Description Document
Lithography SMASH Sensor Objective Design Description Document Zhaoyu Nie (Project Manager) Zichan Wang (Customer Liaison) Yunqi Li (Document) Customer: Hong Ye (ASML) Faculty Advisor: Julie Bentley Graduate
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 informationComputer Generated Holograms for Optical Testing
Computer Generated Holograms for Optical Testing Dr. Jim Burge Associate Professor Optical Sciences and Astronomy University of Arizona jburge@optics.arizona.edu 520-621-8182 Computer Generated Holograms
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 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 informationUser s Guide Modulator Alignment Procedure
User s Guide Modulator Alignment Procedure Models 350, 360, 370, 380, 390 series Warranty Information ConOptics, Inc. guarantees its products to be free of defects in materials and workmanship for one
More informationARCoptix. Radial Polarization Converter. Arcoptix S.A Ch. Trois-portes Neuchâtel Switzerland Mail: Tel:
ARCoptix Radial Polarization Converter Arcoptix S.A Ch. Trois-portes 18 2000 Neuchâtel Switzerland Mail: info@arcoptix.com Tel: ++41 32 731 04 66 Radially and azimuthally polarized beams generated by Liquid
More informationOptics for the 90 GHz GBT array
Optics for the 90 GHz GBT array Introduction The 90 GHz array will have 64 TES bolometers arranged in an 8 8 square, read out using 8 SQUID multiplexers. It is designed as a facility instrument for the
More informationCollimation Tester Instructions
Description Use shear-plate collimation testers to examine and adjust the collimation of laser light, or to measure the wavefront curvature and divergence/convergence magnitude of large-radius optical
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 informationCHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT
CHAPTER 5 FINE-TUNING OF AN ECDL WITH AN INTRACAVITY LIQUID CRYSTAL ELEMENT In this chapter, the experimental results for fine-tuning of the laser wavelength with an intracavity liquid crystal element
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 informationHandbook of Optical Systems
Handbook of Optical Systems Volume 5: Metrology of Optical Components and Systems von Herbert Gross, Bernd Dörband, Henriette Müller 1. Auflage Handbook of Optical Systems Gross / Dörband / Müller schnell
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 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 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 informationUSE OF COMPUTER- GENERATED HOLOGRAMS IN OPTICAL TESTING
14 USE OF COMPUTER- GENERATED HOLOGRAMS IN OPTICAL TESTING Katherine Creath College of Optical Sciences University of Arizona Tucson, Arizona Optineering Tucson, Arizona James C. Wyant College of Optical
More informationSpectrograph Lens Fabrication RFQ 22 Jan, 2003
Spectrograph Lens Fabrication RFQ 22 Jan, 2003 1 Scope of Project This document describes the specifications for the fabrication of 18 optical elements to be used in the Prime Focus Imaging Spectrograph
More informationPREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES
Page 1 of 34 LIGHTMACHINERY TEST REPORT LQT 30.11-3 TITLE: HMI Michelson Interferometer Test Report Serial Number 3 wide band FSR INSTRUCTION OWNER HMI Project Manager PREPARED BY: I. Miller DATE: 2004
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 informationDesign for a new Prime Focus Corrector on the Wyoming InfraRed Observatory (WIRO) 2.3 m Telescope Final Pre-fabrication design of 12 January, 2004
Design for a new Prime Focus Corrector on the Wyoming InfraRed Observatory (WIRO) 2.3 m Telescope Final Pre-fabrication design of 12 January, 2004 PI: Chip Kobulnicky Department of Physics & Astronomy
More information2.2 Wavefront Sensor Design. Lauren H. Schatz, Oli Durney, Jared Males
Page: 1 of 8 Lauren H. Schatz, Oli Durney, Jared Males 1 Pyramid Wavefront Sensor Overview The MagAO-X system uses a pyramid wavefront sensor (PWFS) for high order wavefront sensing. The wavefront sensor
More informationTutorial Zemax 3 Aberrations
Tutorial Zemax 3 Aberrations 2012-08-14 3 Aberrations 1 3.1 Exercise 3-1: Strehl ratio and geometrical vs Psf spot size... 1 3.2 Exercise 3-2: Performance of an achromate... 3 3.3 Exercise 3-3: Anamorphotic
More informationWaveMaster IOL. Fast and Accurate Intraocular Lens Tester
WaveMaster IOL Fast and Accurate Intraocular Lens Tester INTRAOCULAR LENS TESTER WaveMaster IOL Fast and accurate intraocular lens tester WaveMaster IOL is an instrument providing real time analysis of
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 informationLocalized Slope Errors and their impact on image performance requirements
Localized Slope Errors and their impact on image performance requirements Mark C. Sanson, C. Theodore Tienvieri, and Steven VanKerkhove Corning Tropel Corporation, 6 O Connor Road, Fairport, NY 1445 SansonMC@corning.com,
More informationEE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name:
EE119 Introduction to Optical Engineering Fall 2009 Final Exam Name: SID: CLOSED BOOK. THREE 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental
More informationUser s Guide Modulator Alignment Procedure
User s Guide Modulator Alignment Procedure Models 350, 360, 370, 380, 390 series Warranty Information Conoptics, Inc. guarantees its products to be free of defects in materials and workmanship for one
More informationMechanical Tolerancing Results For the SALT/PFIS Collimator and Camera. January 24, 2003 J. Alan Schier
Mechanical Tolerancing Results For the SALT/PFIS Collimator and Camera January 24, 2003 J. Alan Schier This report contains the tolerance information needed to produce a mechanical design for the SALT/PFIS
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 informationAdvanced Dimensional Management LLC
Index: Mechanical Tolerance Stackup and Analysis Bryan R. Fischer Accuracy and precision 8-9 Advanced Dimensional Management 14, 21, 78, 118, 208, 251, 286, 329-366 Ambiguity 4, 8-14 ASME B89 48 ASME Y14.5M-1994
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 informationChapter Ray and Wave Optics
109 Chapter Ray and Wave Optics 1. An astronomical telescope has a large aperture to [2002] reduce spherical aberration have high resolution increase span of observation have low dispersion. 2. If two
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 informationAlex Lyubarsky OPTI 521 December 8, 2013
Alex Lyubarsky OPTI 521 December 8, 2013 Introduction to Optical Specification Standards (Section 1) Sections 2-13 of ISO 10110 Standard Specification ISO 10110 Drawings Q & A ISO 10110 standard created
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 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 informationFizeau interferometer with spherical reference and CGH correction for measuring large convex aspheres
Fizeau interferometer with spherical reference and CGH correction for measuring large convex aspheres M. B. Dubin, P. Su and J. H. Burge College of Optical Sciences, The University of Arizona 1630 E. University
More informationDesign of null lenses for testing of elliptical surfaces
Design of null lenses for testing of elliptical surfaces Yeon Soo Kim, Byoung Yoon Kim, and Yun Woo Lee Null lenses are designed for testing the oblate elliptical surface that is the third mirror of the
More informationInfra Red Interferometers
Infra Red Interferometers for performance testing of infra-red materials and optical systems Specialist expertise in testing, analysis, design, development and manufacturing for Optical fabrication, Optical
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 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 informationABSTRACT. Keywords: Computer-aided alignment, Misalignments, Zernike polynomials, Sensitivity matrix 1. INTRODUCTION
Computer-Aided Alignment for High Precision Lens LI Lian, FU XinGuo, MA TianMeng, WANG Bin The institute of optical and electronics, the Chinese Academy of Science, Chengdu 6129, China ABSTRACT Computer-Aided
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 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 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 informationAgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%.
Application Note AN004: Fiber Coupling Improvement Introduction AgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%. Industrial lasers used for cutting, welding, drilling,
More informationCHAPTER 1 OPTIMIZATION
CHAPTER 1 OPTIMIZATION For the first 40 years of the twentieth century, optical design was done using a mixture of Seidel theory, a little ray tracing, and a great deal of experimental work. All of the
More informationEvaluation of Performance of the Toronto Ultra-Cold Atoms Laboratory s Current Axial Imaging System
Page 1 5/7/2007 Evaluation of Performance of the Toronto Ultra-Cold Atoms Laboratory s Current Axial Imaging System Vincent Kan May 7, 2007 University of Toronto Department of Physics Supervisor: Prof.
More informationFinite conjugate spherical aberration compensation in high numerical-aperture optical disc readout
Finite conjugate spherical aberration compensation in high numerical-aperture optical disc readout Sjoerd Stallinga Spherical aberration arising from deviations of the thickness of an optical disc substrate
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 information