Optical Design with Zemax

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

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

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

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

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

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

Optical Design with Zemax for PhD - Basics

Optical Design with Zemax

Lens Design I Seminar 1

Optical Design with Zemax for PhD

Advanced Lens Design

Tutorial Zemax 8: Correction II

Solution of Exercises Lecture Optical design with Zemax for PhD Part 8

Solution of Exercises Lecture Optical design with Zemax Part 6

Exercises Advanced Optical Design Part 5 Solutions

Solutions: Lens Design I Part 2. Exercise 2-1: Apertures, stops and vignetting

Optical Design with Zemax for PhD

Advanced Lens Design

Tutorial Zemax 3 Aberrations

Tutorial Zemax Introduction 1

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

Lens Design I Seminar 5

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

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

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

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

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

Exercise 1 - Lens bending

Lens Design II Seminar 6 (Solutions)

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

System/Prescription Data

Optical Design with Zemax

GEOMETRICAL OPTICS AND OPTICAL DESIGN

Exam Preparation Guide Geometrical optics (TN3313)

OPTICAL IMAGING AND ABERRATIONS

Lens Design II. Lecture 3: Aspheres Herbert Gross. Winter term

Sequential Ray Tracing. Lecture 2


Lens Design II. Lecture 8: Special correction topics Herbert Gross. Winter term

Mechanical Tolerancing Results For the SALT/PFIS Collimator and Camera. January 24, 2003 J. Alan Schier

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

3.0 Alignment Equipment and Diagnostic Tools:

Chapter 3. Introduction to Zemax. 3.1 Introduction. 3.2 Zemax

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

Tutorial Zemax 9: Physical optical modelling I

ECEN 4606, UNDERGRADUATE OPTICS LAB

Phys 531 Lecture 9 30 September 2004 Ray Optics II. + 1 s i. = 1 f

Lens Design II. Lecture 8: Special correction features I Herbert Gross. Winter term

Design and Correction of optical Systems

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

Long Wave Infrared Scan Lens Design And Distortion Correction

Imaging and Aberration Theory

Lens Design II. Lecture 3: Aspheres Herbert Gross. Winter term

Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California

Optical Engineering 421/521 Sample Questions for Midterm 1

Microscopy. Lecture 2: Optical System of the Microscopy II Herbert Gross. Winter term

October 7, Peter Cheimets Smithsonian Astrophysical Observatory 60 Garden Street, MS 5 Cambridge, MA Dear Peter:

ME 297 L4-2 Optical design flow Analysis

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

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)

Opti 415/515. Introduction to Optical Systems. Copyright 2009, William P. Kuhn

Parity and Plane Mirrors. Invert Image flip about a horizontal line. Revert Image flip about a vertical line.

Metrology and Sensing

Why is There a Black Dot when Defocus = 1λ?

Some lens design methods. Dave Shafer David Shafer Optical Design Fairfield, CT #

CHAPTER 33 ABERRATION CURVES IN LENS DESIGN

Geometric optics & aberrations

Ch 24. Geometric Optics

Optimisation. Lecture 3

CATALOG LENS USE IN OSLO

Handbook of Optical Systems

Lecture 3: Geometrical Optics 1. Spherical Waves. From Waves to Rays. Lenses. Chromatic Aberrations. Mirrors. Outline

OPTICAL SYSTEMS OBJECTIVES

Lecture 8. Lecture 8. r 1

TOPICS Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization

Optical System Design

CHAPTER 1 Optical Aberrations

Computer exercise 2 geometrical optics and the telescope

Properties of optical instruments

Lens Design II. Lecture 8: Special correction features I Herbert Gross. Winter term

INTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS

Using Stock Optics. ECE 5616 Curtis

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

Design of a Lens System for a Structured Light Projector

Introductions to aberrations OPTI 517

Chapter 34 Geometric Optics (also known as Ray Optics) by C.-R. Hu

Evaluation of Performance of the Toronto Ultra-Cold Atoms Laboratory s Current Axial Imaging System

Magnification, stops, mirrors More geometric optics

Performance Factors. Technical Assistance. Fundamental Optics

Properties of optical instruments. Visual optical systems part 2: focal visual instruments (microscope type)

Waves & Oscillations

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

Index. B Back focal length, 12 Beam expander, 35 Berek, Max, 244 Binary phase grating, 326 Buried surface, 131,

Optical Design of. Microscopes. George H. Seward. Tutorial Texts in Optical Engineering Volume TT88. SPIE PRESS Bellingham, Washington USA

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

Chapter 3 Op,cal Instrumenta,on

Supplemental Materials. Section 25. Aberrations

PROCEEDINGS OF SPIE. Measurement of low-order aberrations with an autostigmatic microscope

Lithography Smash Sensor Objective Product Requirements Document

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

Transcription:

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 I 3 02.05. Properties of optical systems II 4 09.05. Aberrations I Introduction, Zemax interface, menues, file handling, preferences, Editors, updates, windows, coordinates, System description, Component reversal, system insertion, scaling, 3D geometry, aperture, field, wavelength Diameters, stop and pupil, vignetting, Layouts, Materials, Glass catalogs, Raytrace, Ray fans and sampling, Footprints Types of surfaces, Aspheres, Gratings and diffractive surfaces, Gradient media, Cardinal elements, Lens properties, Imaging, magnification, paraxial approximation and modelling Representation of geometrical aberrations, Spot diagram, Transverse aberration diagrams, Aberration expansions, Primary aberrations, 5 16.05. Aberrations II Wave aberrations, Zernike polynomials 6 23.05. Aberrations III Point spread function, Optical transfer function 7 30.05. Optimization I Principles of nonlinear optimization, Optimization in optical design, Global optimization methods, Solves and pickups, variables, Sensitivity of variables in optical systems 8 06.06. Optimization II Systematic methods and optimization process, Starting points, Optimization in Zemax 9 13.06. Advanced handling I Telecentricity, infinity object distance and afocal image, Local/global coordinates, Add fold mirror, Scale system, Make double pass, Vignetting, Diameter types, Ray aiming, Material index fit 10 20.06. Advanced handling II Report graphics, Universal plot, Slider, Visual optimization, IO of data, Multiconfiguration, Fiber coupling, Macro language, Lens catalogs 11 27.06. Imaging Fundamentals of Fourier optics, Physical optical image formation, Imaging in Zemax 12 04.07. Correction I 13 11.07. Correction II Symmetry principle, Lens bending, Correcting spherical aberration, Coma, stop position, Astigmatism, Field flattening, Chromatical correction, Retrofocus and telephoto setup, Design method Field lenses, Stop position influence, Aspheres and higher orders, Principles of glass selection, Sensitivity of a system correction

3 Contents 1. Miscellaneous 2. Vignetting, diameter types, ray aiming 3. Material index fit 4. Lens catalogs

4 Special Infinity Cases Object in infinity - incoming marginal ray parallel to axis - first distance infinity - off-axis field only as angle - no initial NA possible Image in infinity - outgoing marginal ray ideally parallel to axis - explicit declaration: afocal image space - geometrical aberrations as angles - wave aberration reference is plane wave - definition of Airy diameter in mrad Entrance pupil in infinity - incoming chief ray parallel to axis - explicit declaration: telecentric object space Exit pupil in infinity - outgoing chief ray ideally parallel to axis

The Special Infinity Cases Simple case: - object, image and pupils are lying in a finite distance - non-telecentric relay systems Special case 1: - object at infinity - object sided afocal - example: camera lens for distant objects Special case 2: - image at infinity - image sided afocal - example: eyepiece Special case 3: - exit pupil at infinity - image side telecentric - example: camera lens for metrology Special case 4: - exit pupil at infinity - image sided telecentric - example: old fashion lithographic lens 5

The Special Infinity Cases Very special: combination of above cases Examples: - both sided telecentric: 4f-system, lithographic lens - both sided afocal: afocal zoom - object sided telecentric, image sided afocal: microscopic lens Notice: telecentricity and afocality can not be combined on the same side of a system

7 Cardinal Elements in Zemax Cardinal elements of a selected index range (lens or group)

8 Quick Focus Option In the menue TOOLS DESIGN QUICK FOCUS we have the opportunity to adjust the image location according to the criteria 1. Spot diameter 2. Wavefront rms 3. Angle radius IN principle, this option is a simplified optimization Example: find the best image plane of a single lens Spot before and after performing the optimal focussing

9 Quick Adjust Option In the menue TOOLS DESIGN QUICK ADJUST we have the opportunity to adjust 1. one thickness 2. one radius similar to the quick focus function some where in the system Special application: adjust the air distance before a collimation lens to get the best collimation As criteria, wavefroint, spot diameter of angular radius ar possible Example: Move a lens in between a system to focus the image Spots before and aftre thew adjustment

10 System changes Useful commands for system changes: 1. Scaling (e.g. patents) 2. Insert system with other system file File - Insert Lens 2. Reverse system

11 3D Geometry Auxiliary menus: 1. Tilt/Decenter element 2. Folding mirror

12 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

Aperture data in Zemax Different possible options for specification of the aperture in Zemax: 1. Entrance pupil diameter 2. Image space F# 3. Object space NA 4. Paraxial working F# 5. Object cone angle 6. Floating by stop size Stop location: 1. Fixes the chief ray intersection point 2. input not necessary for telecentric object space 3. is used for aperture determination in case of aiming Special cases: 1. Object in infinity (NA, cone angle input impossible) 2. Image in infinity (afocal) 3. Object space telecentric

14 Diameters in Zemax There are several different types of diameters in Zemax: 1. Surface stop - defines the axis intersection of the chief ray - usually no influence on aperture size - only one stop in the system - is indicated in the Lens Data Editor by STO - if the initial aperture is defined, the size of the stop semi-diameter is determined by marginal raytrace

15 Diameters in Zemax 2. Userdefined diameter at a surface in the Lens Data Editor (U) - serves also as drawing size in the layout (for nice layouts) - if the diameter in the stop plane is fixed, the initial aperture can be computed automatically by General / Aperture Type / Float by Stop Size This corresponds to a ray aiming 3. Individual diameter of perhaps complicated shape at every surface ( apertures ) - no impact on the drawing - is indicated in the Lens Data Editor by a star - the drawing of vignetted rays can by switched on/off

Diameters and stop sizes 4. Individual aperture sizes for every field point can be set by the vignetting factors of the Field menu - real diameters at surfaces must be set - reduces light cones are drawn in the layout VDX, VDY: relative decenter of light cone in x, y VCX, VCY: compressian factors in x, y VAN: azimuthal rotation angle of light cone - If limiting diameters are set in the system, the corresponding factors can be calculated by the Set Vig command 16

17 Diameters in Zemax In the Tools-menue, the diameters and apertures can be converted automatically

18 Ray Aiming Userdefined diameter at a surface in the Lens Data Editor (U) - serves also as drawing size in the layout (for nice layouts) - if the diameter of the system stop is fixed, the initial aperture can be computed automatically by General / Aperture Type / Float by Stop Size This corresponds to a ray aiming on the rim of the stop surface. The aperture values in the PRESCRIPTION DATA list then changes with the diameter A more general aiming and determination of the opening for all predefined diameters is not possible in Zemax

Material Index Fit choice of 4 dispersion formula after fit: - pv and rms of approximation visible - no individual errors seen check results for suitable accuracy, especially at wavelengths and temperatures with sparse input data and at intervall edges add to catalog enter additional data Save catalog Ref.: B. Böhme 19

20 Material Index Fit Establishing a special own material Select menue: Tools / Catalogs / Glass catalogs Options: 1. Fit index data 2. Fit melt data Input of data for wavelengths and indices It is possible to establish own material catalogs with additional glasses as an individual library

21 Material Index Fit Melt data: - for small differences of real materials - no advantage for new materials Menue option: Glass Fitting Tool don t works (data input?)

22 Material Index Fit Menue: Fit Index Data Input of data: 2 options: 1. explicite entering wavelengths and indices 2. load file xxx.dat with two columns: wavelength in mm and index Choice of 4 different dispersion formulas After fit: - pv and rms of approximation visible - no individual errors seen - new material can be added to catalog - data input can be saved to file

Lens Catalogs Lens catalogs: Data of commercial lens vendors Searching machine for one vendor Componenets can be loaded or inserted Preview and data prescription possible Special code of components in brackets according to search criteria 23

Lens Catalogs Some system with more than one lens available Sometimes: - aspherical constants wrong - hidden data with diameters, wavelengths,... - problems with old glasses Data stored in binary.zmf format Search over all catalogs not possible Catalogs changes dynamically with every release Private catalog can be generated 24

Stock Lens Matching This tool swaps out lenses in a design to the nearest equivalent candidate out of a vendor catalogue It works together with the merit function requirements (with constraints) Aspheric, GRIN and toroidal surfaces not supported; only spherical Works for single lenses and achromates Compensation due to thickness adjustments is optional Reverting a lens to optimize (?) Top results are listed Combination of best single lens substitutions is possible. Overall optimization with nonlinear interaction? Ref.: D. Lokanathan

Stock Lens Matching Selectioin of some vendors by CNTR SHIFT marking Ref.: D. Lokanathan

Stock Lens Matching Output Ref.: D. Lokanathan