Introduction to aberrations

Size: px
Start display at page:

Download "Introduction to aberrations"

Transcription

1 Introduction to aberrations Lecture 8 Image and aberration evaluation 1

2 Aberrations and image: Aberration theory Aberration evaluation Image formation Image evaluation Geometrical and physical theories The image of a point object

3 Criteria The application determines the aberration tolerances Most usually the detector pixel size or the specification on resolution The case of visual instruments 3

4 Resolution Resolution is an important image quality metric It determines whether two closely spaced, and equal irradiance, objects can be identified as two mm Well resolved mm 5 Rayleigh resolution peak of nd at 1st zero of first 4

5 Resolution 5

6 Rules that rule optics RES k ; DOF k NA n NA 1 Wavelength=193nm k1~ Raleigh resolution k1=0.61 K~0.5 R(193 dry)=147nm (NA=0.8; k1=0.61) DOF=151 nm Must preserve imaging volume! Resolution and depth of focus are critical. R(193 water)=110 nm 6

7 Diffraction Encircled Energy in the Airy pattern % % 0.8 ENCIRCLED ENERGY st zero nd zero DIAMETER OF CIRCLE (MM) 7

8 8

9 9

10 10

11 Aberration balancing 11

12 Wavefront variance in the presence of primary aberrations 1

13 Rayleigh-Strehl ratio 13

14 Rayleigh-Strehl ratio 14

15 Use of the central-ordinate theorem 15

16 16

17 17

18 Andre Marechal formula I W I 1 1 W 18

19 Shack s formula I W I exp W 19

20 Shack s formula derivation 0

21 Shack s formula derivation cont. Given by an OPTI518 student 1

22 Rayleigh-Strehl ratio Rayleigh Strehl Aberrated PSF peak Unaberrated PSF peak See Lord Rayleigh, Investigations in optics, with special reference to the spectroscope, Phil. Mag. Vol. 5(8), , Strehl, K. 1895, Aplanatische und fehlerhafte Abbildung im Fernrohr, Zeitschrift für Instrumentenkunde 15 (Oct.), Strehl, K. 190, Über Luftschlieren und Zonenfehler, Zeitschrift für Instrumentenkunde, (July), V. N. Mahajan, Strehl ratio for primary aberrations in terms of their aberration variance, J. Opt. Soc. Am. Vol. 73(6) , 1983.

23 Rayleigh-Strehl ratio S ~1 w S ~ e w Approximation Good for S~>0.3 Good for S~>0.1 It is the variance of the wavefront deformation 3

24 Some Rayleigh-Strehl ratio insights Ratio of aberrated to unaberrated PSF peaks Scattered energy Contributions form refracting and reflecting surfaces Contributions from rough surfaces DOE efficiency Keep in mind formula limits S ~1 w 4

25 The case of refraction vs. reflection surface S ~1 1 n' n w n' n 0.5 refraction n' n 4 reflection Ratio of scattered energy is 16! Thus for a given surface roughness, reflection scatters 16 times more than refraction. Note dependence with wavelength 5

26 Marechal Criterion ~1947 Keep in mind that is not only the resolution but also the depth of focus. MUST PRESERVE ALL DOF!!! 6

27 Best focus according to variance W W

28 The concept of Diffraction limited Not limited by geometrical aberrations Depends on the particular technical field Usually means RSR > 0.8 A healthy human eye is diffraction limited at a pupil diameter of ~ 1.5 mm 8

29 Roland Shack s notes 9

30 Binocular quality Inexpensive binos Expensive binos 4X10 Double pass Double pass Spherical aberration in the eye: ~+4 waves for a 6 mm pupil at 587 nm. Or ¼ wave for a 3 mm pupil. 30

31 Topics Aberration/image evaluation Image of a point object Rules that rule the optics world Wavefront variance Aberration balancing Raleigh-Strehl ratio 31

Lens Design I Seminar 5

Lens Design I Seminar 5 Y. Sekman, X. Lu, H. Gross Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design I Seminar 5 Exercise 5-1: PSF scaling (Homework) To check the Airy

More information

Optics of Wavefront. Austin Roorda, Ph.D. University of Houston College of Optometry

Optics of Wavefront. Austin Roorda, Ph.D. University of Houston College of Optometry Optics of Wavefront Austin Roorda, Ph.D. University of Houston College of Optometry Geometrical Optics Relationships between pupil size, refractive error and blur Optics of the eye: Depth of Focus 2 mm

More information

( ) Deriving the Lens Transmittance Function. Thin lens transmission is given by a phase with unit magnitude.

( ) Deriving the Lens Transmittance Function. Thin lens transmission is given by a phase with unit magnitude. Deriving the Lens Transmittance Function Thin lens transmission is given by a phase with unit magnitude. t(x, y) = exp[ jk o ]exp[ jk(n 1) (x, y) ] Find the thickness function for left half of the lens

More information

Tutorial Zemax 3 Aberrations

Tutorial 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 information

Binocular and Scope Performance 57. Diffraction Effects

Binocular and Scope Performance 57. Diffraction Effects Binocular and Scope Performance 57 Diffraction Effects The resolving power of a perfect optical system is determined by diffraction that results from the wave nature of light. An infinitely distant point

More information

INTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS

INTRODUCTION 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 information

Diffraction of a Circular Aperture

Diffraction of a Circular Aperture DiffractionofaCircularAperture Diffraction can be understood by considering the wave nature of light. Huygen's principle, illustrated in the image below, states that each point on a propagating wavefront

More information

MICRO AND NANOPROCESSING TECHNOLOGIES

MICRO AND NANOPROCESSING TECHNOLOGIES MICRO AND NANOPROCESSING TECHNOLOGIES LECTURE 4 Optical lithography Concepts and processes Lithography systems Fundamental limitations and other issues Photoresists Photolithography process Process parameter

More information

Review of Basic Principles in Optics, Wavefront and Wavefront Error

Review of Basic Principles in Optics, Wavefront and Wavefront Error Review of Basic Principles in Optics, Wavefront and Wavefront Error Austin Roorda, Ph.D. University of California, Berkeley Google my name to find copies of these slides for free use and distribution Geometrical

More information

Modulation Transfer Function

Modulation Transfer Function Modulation Transfer Function The Modulation Transfer Function (MTF) is a useful tool in system evaluation. t describes if, and how well, different spatial frequencies are transferred from object to image.

More information

12.4 Alignment and Manufacturing Tolerances for Segmented Telescopes

12.4 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 information

Shaping light in microscopy:

Shaping light in microscopy: Shaping light in microscopy: Adaptive optical methods and nonconventional beam shapes for enhanced imaging Martí Duocastella planet detector detector sample sample Aberrated wavefront Beamsplitter Adaptive

More information

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

Applied Optics. , Physics Department (Room #36-401) , , Applied Optics Professor, Physics Department (Room #36-401) 2290-0923, 019-539-0923, shsong@hanyang.ac.kr Office Hours Mondays 15:00-16:30, Wednesdays 15:00-16:30 TA (Ph.D. student, Room #36-415) 2290-0921,

More information

CCAM s Selection of. Zeiss Microscope Objectives

CCAM s Selection of. Zeiss Microscope Objectives CCAM s Selection of Zeiss Microscope Objectives 1. Magnification Image scale 2. Resolution The minimum separation distance between two points that are clearly resolved. The resolution of an objective is

More information

Study on Imaging Quality of Water Ball Lens

Study on Imaging Quality of Water Ball Lens 2017 2nd International Conference on Mechatronics and Information Technology (ICMIT 2017) Study on Imaging Quality of Water Ball Lens Haiyan Yang1,a,*, Xiaopan Li 1,b, 1,c Hao Kong, 1,d Guangyang Xu and1,eyan

More information

Lecture Notes 10 Image Sensor Optics. Imaging optics. Pixel optics. Microlens

Lecture Notes 10 Image Sensor Optics. Imaging optics. Pixel optics. Microlens Lecture Notes 10 Image Sensor Optics Imaging optics Space-invariant model Space-varying model Pixel optics Transmission Vignetting Microlens EE 392B: Image Sensor Optics 10-1 Image Sensor Optics Microlens

More information

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

Optical Design of. Microscopes. George H. Seward. Tutorial Texts in Optical Engineering Volume TT88. SPIE PRESS Bellingham, Washington USA Optical Design of Microscopes George H. Seward Tutorial Texts in Optical Engineering Volume TT88 SPIE PRESS Bellingham, Washington USA Preface xiii Chapter 1 Optical Design Concepts /1 1.1 A Value Proposition

More information

Lecture 8. Lecture 8. r 1

Lecture 8. Lecture 8. r 1 Lecture 8 Achromat Design Design starts with desired Next choose your glass materials, i.e. Find P D P D, then get f D P D K K Choose radii (still some freedom left in choice of radii for minimization

More information

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)

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) 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 information

Optical Design of an Off-axis Five-mirror-anastigmatic Telescope for Near Infrared Remote Sensing

Optical Design of an Off-axis Five-mirror-anastigmatic Telescope for Near Infrared Remote Sensing Journal of the Optical Society of Korea Vol. 16, No. 4, December 01, pp. 343-348 DOI: http://dx.doi.org/10.3807/josk.01.16.4.343 Optical Design of an Off-axis Five-mirror-anastigmatic Telescope for Near

More information

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

The Brownie Camera. Lens Design OPTI 517. Prof. Jose Sasian The Brownie Camera Lens Design OPTI 517 http://www.history.roch ester.edu/class/kodak/k odak.htm George Eastman (1854-1932), was an ingenious man who contributed greatly to the field of photography. He

More information

Point-spread Function modeling for the James Webb Space Telescope

Point-spread Function modeling for the James Webb Space Telescope Point-spread Function modeling for the James Webb Space Telescope Colin Cox and Philip Hodge Space Telescope Science Institute 9 November 2006 Leads Meeting 1 Objectives Provide a model of the JWST PSF

More information

Tutorial Zemax 8: Correction II

Tutorial 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 information

Wavefront Sensing Under Unique Lighting Conditions

Wavefront Sensing Under Unique Lighting Conditions Wavefront Sensing Under Unique Lighting Conditions Shack-Hartmann wavefront sensors prove critical in detecting light propagation properties of noncoherent light sources. BY JOHANNES PFUND, RALF DORN and

More information

Limits of Higher Order Correction based on Spot Size, Ablation Depth, and Tracker Responsiveness

Limits of Higher Order Correction based on Spot Size, Ablation Depth, and Tracker Responsiveness Limits of Higher Order Correction based on Spot Size, Ablation Depth, and Tracker Responsiveness Michael Bueeler a,b, Michael Mrochen a,b, Theo Seiler b a Swiss Federal Institute of Technology Zurich,

More information

Confocal Imaging Through Scattering Media with a Volume Holographic Filter

Confocal Imaging Through Scattering Media with a Volume Holographic Filter Confocal Imaging Through Scattering Media with a Volume Holographic Filter Michal Balberg +, George Barbastathis*, Sergio Fantini % and David J. Brady University of Illinois at Urbana-Champaign, Urbana,

More information

Predicting the Performance of Space Coronagraphs. John Krist (JPL) 17 August st International Vortex Workshop

Predicting the Performance of Space Coronagraphs. John Krist (JPL) 17 August st International Vortex Workshop Predicting the Performance of Space Coronagraphs John Krist (JPL) 17 August 2016 1 st International Vortex Workshop Determine the Reality of a Coronagraph through End-to-End Modeling Use End-to-End modeling

More information

Ron Liu OPTI521-Introductory Optomechanical Engineering December 7, 2009

Ron Liu OPTI521-Introductory Optomechanical Engineering December 7, 2009 Synopsis of METHOD AND APPARATUS FOR IMPROVING VISION AND THE RESOLUTION OF RETINAL IMAGES by David R. Williams and Junzhong Liang from the US Patent Number: 5,777,719 issued in July 7, 1998 Ron Liu OPTI521-Introductory

More information

What is the source of straylight in SST/CRISP data?

What is the source of straylight in SST/CRISP data? What is the source of straylight in SST/CRISP data? G.B. Scharmer* with Mats Löfdahl, Dan Kiselman, Marco Stangalini Based on: Scharmer et al., A&A 521, A68 (2010) Löfdahl & Scharmer, A&A 537, A80 (2012)

More information

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

1.1 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 information

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

October 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 information

Handbook of Optical Systems

Handbook 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 information

Strehl ratio for primary aberrations: some analytical results for circular and annular pupils

Strehl ratio for primary aberrations: some analytical results for circular and annular pupils 1258 J. Opt. Soc. Am./Vol. 72, No. 9/September 1982 Strehl ratio for primary aberrations: some analytical results for circular and annular pupils The Charles Stark Draper Laboratory, Inc., Cambridge, Massachusetts

More information

HOYA aspherical IOL with ABC (Aspheric Balanced Curve) Design

HOYA aspherical IOL with ABC (Aspheric Balanced Curve) Design HOYA aspherical IOL with ABC (Aspheric Balanced Curve) Design Contents Basics of asphericity Visual quality and aspheric IOL Features of HOYA ABC Design 2 What is asphericity? Deviating from the spherical

More information

On Maximization of Strehl-Ratio and Minimization of Second-Order Moment in the Green s Functions of Apodised Optical Systems

On Maximization of Strehl-Ratio and Minimization of Second-Order Moment in the Green s Functions of Apodised Optical Systems Journal of Emerging Trends in Engineering and Applied Sciences (JETEAS) 5(): 6- Scholarlink Research Institute Journals, 4 (ISSN: 4-76) jeteas.scholarlinkresearch.org Journal of Emerging Trends in Engineering

More information

3.0 Alignment Equipment and Diagnostic Tools:

3.0 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 information

LECTURE 13 DIFFRACTION. Instructor: Kazumi Tolich

LECTURE 13 DIFFRACTION. Instructor: Kazumi Tolich LECTURE 13 DIFFRACTION Instructor: Kazumi Tolich Lecture 13 2 Reading chapter 33-4 & 33-6 to 33-7 Single slit diffraction Two slit interference-diffraction Fraunhofer and Fresnel diffraction Diffraction

More information

Wavefront control for highcontrast

Wavefront control for highcontrast Wavefront control for highcontrast imaging Lisa A. Poyneer In the Spirit of Bernard Lyot: The direct detection of planets and circumstellar disks in the 21st century. Berkeley, CA, June 6, 2007 p Gemini

More information

Design considerations for low-light level low-fresnel number optical systems

Design considerations for low-light level low-fresnel number optical systems Design considerations for low-light level low-fresnel number optical systems Christoph Baranec Caltech Optical Observatories, California Institute of Technology, 1200 East California Boulevard, Pasadena,

More information

OPTI 517 Image Quality. Richard Juergens

OPTI 517 Image Quality. Richard Juergens OPTI 517 Image Quality Richard Juergens 520-577-6918 rcjuergens@msn.com Why is Image Quality Important? Resolution of detail Smaller blur sizes allow better reproduction of image details Addition of noise

More information

Wavefront Sensing In Other Disciplines. 15 February 2003 Jerry Nelson, UCSC Wavefront Congress

Wavefront Sensing In Other Disciplines. 15 February 2003 Jerry Nelson, UCSC Wavefront Congress Wavefront Sensing In Other Disciplines 15 February 2003 Jerry Nelson, UCSC Wavefront Congress QuickTime and a Photo - JPEG decompressor are needed to see this picture. 15feb03 Nelson wavefront sensing

More information

Properties of optical instruments. Projection optical systems

Properties of optical instruments. Projection optical systems Properties of optical instruments Projection optical systems Instruments : optical systems designed for a specific function Projection systems: : real image (object real or at infinity) Examples: videoprojector,,

More information

Metrology and Sensing

Metrology and Sensing Metrology and Sensing Lecture 7: Wavefront sensors 2016-11-29 Herbert Gross Winter term 2016 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed Content 1 18.10. Introduction Introduction,

More information

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

Cardinal Points of an Optical System--and Other Basic Facts Cardinal Points of an Optical System--and Other Basic Facts The fundamental feature of any optical system is the aperture stop. Thus, the most fundamental optical system is the pinhole camera. The image

More information

Subjective Image Quality Metrics from The Wave Aberration

Subjective Image Quality Metrics from The Wave Aberration Subjective Image Quality Metrics from The Wave Aberration David R. Williams William G. Allyn Professor of Medical Optics Center For Visual Science University of Rochester Commercial Relationship: Bausch

More information

Chapter 1. Basic Electron Optics (Lecture 2)

Chapter 1. Basic Electron Optics (Lecture 2) Chapter 1. Basic Electron Optics (Lecture 2) Basic concepts of microscope (Cont ) Fundamental properties of electrons Electron Scattering Instrumentation Basic conceptions of microscope (Cont ) Ray diagram

More information

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

Microscopy. Lecture 2: Optical System of the Microscopy II Herbert Gross. Winter term Microscopy Lecture 2: Optical System of the Microscopy II 212-1-22 Herbert Gross Winter term 212 www.iap.uni-jena.de Preliminary time schedule 2 No Date Main subject Detailed topics Lecturer 1 15.1. Optical

More information

Supplementary Information for: Immersion Meta-lenses at Visible Wavelengths for Nanoscale Imaging

Supplementary Information for: Immersion Meta-lenses at Visible Wavelengths for Nanoscale Imaging Supplementary Information for: Immersion Meta-lenses at Visible Wavelengths for Nanoscale Imaging Wei Ting Chen 1,, Alexander Y. Zhu 1,, Mohammadreza Khorasaninejad 1, Zhujun Shi 2, Vyshakh Sanjeev 1,3

More information

Optical Design with Zemax for PhD - Basics

Optical 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 information

Dynamic beam shaping with programmable diffractive optics

Dynamic beam shaping with programmable diffractive optics Dynamic beam shaping with programmable diffractive optics Bosanta R. Boruah Dept. of Physics, GU Page 1 Outline of the talk Introduction Holography Programmable diffractive optics Laser scanning confocal

More information

CCAM Microscope Objectives

CCAM Microscope Objectives CCAM Microscope Objectives Things to consider when selecting an objective Magnification Numerical Aperture (NA) resolving power and light intensity of the objective Working Distance distance between the

More information

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

Design of Large Working Area F-Theta Lens. Gong Chen 1 Design of Large Working Area F-Theta Lens by Gong Chen 2 ABSTRACT F-Theta lenses are different from normal camera lenses. It is one of the most important parts of laser scanning system. Besides, F-Theta

More information

Resolution. [from the New Merriam-Webster Dictionary, 1989 ed.]:

Resolution. [from the New Merriam-Webster Dictionary, 1989 ed.]: Resolution [from the New Merriam-Webster Dictionary, 1989 ed.]: resolve v : 1 to break up into constituent parts: ANALYZE; 2 to find an answer to : SOLVE; 3 DETERMINE, DECIDE; 4 to make or pass a formal

More information

High resolution extended depth of field microscopy using wavefront coding

High resolution extended depth of field microscopy using wavefront coding High resolution extended depth of field microscopy using wavefront coding Matthew R. Arnison *, Peter Török #, Colin J. R. Sheppard *, W. T. Cathey +, Edward R. Dowski, Jr. +, Carol J. Cogswell *+ * Physical

More information

Chapter 34 The Wave Nature of Light; Interference. Copyright 2009 Pearson Education, Inc.

Chapter 34 The Wave Nature of Light; Interference. Copyright 2009 Pearson Education, Inc. Chapter 34 The Wave Nature of Light; Interference 34-7 Luminous Intensity The intensity of light as perceived depends not only on the actual intensity but also on the sensitivity of the eye at different

More information

Exercise 1 - Lens bending

Exercise 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 information

Chapter 28 Physical Optics: Interference and Diffraction

Chapter 28 Physical Optics: Interference and Diffraction Chapter 28 Physical Optics: Interference and Diffraction 1 Overview of Chapter 28 Superposition and Interference Young s Two-Slit Experiment Interference in Reflected Waves Diffraction Resolution Diffraction

More information

Reflectors vs. Refractors

Reflectors vs. Refractors 1 Telescope Types - Telescopes collect and concentrate light (which can then be magnified, dispersed as a spectrum, etc). - In the end it is the collecting area that counts. - There are two primary telescope

More information

CHAPTER TWO METALLOGRAPHY & MICROSCOPY

CHAPTER TWO METALLOGRAPHY & MICROSCOPY CHAPTER TWO METALLOGRAPHY & MICROSCOPY 1. INTRODUCTION: Materials characterisation has two main aspects: Accurately measuring the physical, mechanical and chemical properties of materials Accurately measuring

More information

Chapter 25. Optical Instruments

Chapter 25. Optical Instruments Chapter 25 Optical Instruments Optical Instruments Analysis generally involves the laws of reflection and refraction Analysis uses the procedures of geometric optics To explain certain phenomena, the wave

More information

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

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

Introduction to Light Microscopy. (Image: T. Wittman, Scripps)

Introduction to Light Microscopy. (Image: T. Wittman, Scripps) Introduction to Light Microscopy (Image: T. Wittman, Scripps) The Light Microscope Four centuries of history Vibrant current development One of the most widely used research tools A. Khodjakov et al. Major

More information

Adaptive Optics lectures

Adaptive Optics lectures Adaptive Optics lectures 2. Adaptive optics Invented in 1953 by H.Babcock Andrei Tokovinin 1 Plan General idea (open/closed loop) Wave-front sensing, its limitations Correctors (DMs) Control (spatial and

More information

Master program "Optical Design"

Master program Optical Design University ITMO, Russia WUT, Poland Department of Applied and Computer Optics Photonics Engineering Division http://zif.mchtr.pw.edu.pl Master program "Optical Design" (ACO Department), St. Petersburg

More information

System Architecting: Defining Optical and Mechanical Tolerances from an Error Budget

System 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 information

Criteria for Optical Systems: Optical Path Difference How do we determine the quality of a lens system? Several criteria used in optical design

Criteria for Optical Systems: Optical Path Difference How do we determine the quality of a lens system? Several criteria used in optical design Criteria for Optical Systems: Optical Path Difference How do we determine the quality of a lens system? Several criteria used in optical design Computer Aided Design Several CAD tools use Ray Tracing (see

More information

Digital Camera Technologies for Scientific Bio-Imaging. Part 2: Sampling and Signal

Digital Camera Technologies for Scientific Bio-Imaging. Part 2: Sampling and Signal Digital Camera Technologies for Scientific Bio-Imaging. Part 2: Sampling and Signal Yashvinder Sabharwal, 1 James Joubert 2 and Deepak Sharma 2 1. Solexis Advisors LLC, Austin, TX, USA 2. Photometrics

More information

Heisenberg) relation applied to space and transverse wavevector

Heisenberg) relation applied to space and transverse wavevector 2. Optical Microscopy 2.1 Principles A microscope is in principle nothing else than a simple lens system for magnifying small objects. The first lens, called the objective, has a short focal length (a

More information

Bioimage Informatics

Bioimage Informatics Bioimage Informatics Lecture 5, Spring 01 Fundamentals of Fluorescence Microscopy (II) Bioimage Data Analysis (I): Basic Operations Lecture 5 January 5, 01 1 Outline Performance metrics of a microscope

More information

4th International Congress of Wavefront Sensing and Aberration-free Refractive Correction ADAPTIVE OPTICS FOR VISION: THE EYE S ADAPTATION TO ITS

4th International Congress of Wavefront Sensing and Aberration-free Refractive Correction ADAPTIVE OPTICS FOR VISION: THE EYE S ADAPTATION TO ITS 4th International Congress of Wavefront Sensing and Aberration-free Refractive Correction (Supplement to the Journal of Refractive Surgery; June 2003) ADAPTIVE OPTICS FOR VISION: THE EYE S ADAPTATION TO

More information

The MCAO module for the E-ELT.

The MCAO module for the E-ELT. The MCAO module for the E-ELT http://www.bo.astro.it/~maory Paolo Ciliegi (INAF Osservatorio Astronomico di Bologna) On behalf of the MAORY Consortium MAORY Consortium INAF BOLOGNA UNIVERSITY ONERA ESO

More information

PHYS 202 OUTLINE FOR PART III LIGHT & OPTICS

PHYS 202 OUTLINE FOR PART III LIGHT & OPTICS PHYS 202 OUTLINE FOR PART III LIGHT & OPTICS Electromagnetic Waves A. Electromagnetic waves S-23,24 1. speed of waves = 1/( o o ) ½ = 3 x 10 8 m/s = c 2. waves and frequency: the spectrum (a) radio red

More information

Lecture Outline Chapter 28. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Lecture Outline Chapter 28. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc. Lecture Outline Chapter 28 Physics, 4 th Edition James S. Walker Chapter 28 Physical Optics: Interference and Diffraction Units of Chapter 28 Superposition and Interference Young s Two-Slit Experiment

More information

Diffraction. modern investigations date from Augustin Fresnel

Diffraction. modern investigations date from Augustin Fresnel Diffraction Diffraction controls the detail you can see in optical instruments, makes holograms, diffraction gratings and much else possible, explains some natural phenomena Diffraction was discovered

More information

PYRAMID WAVEFRONT SENSING UPDATE FOR MAGAO-X

PYRAMID WAVEFRONT SENSING UPDATE FOR MAGAO-X PYRAMID WAVEFRONT SENSING UPDATE FOR MAGAO-X LAUREN H SCHATZ 1, JARED MALES 2, MICHAEL HART 1, LAIRD CLOSE 2, KATIE MORZINSKI 2, OLIVIER GUYON 1,2,3,4, MADISON JEAN 1,CHRIS BOHLMAN 2, KYLE VAN GORKOM 1,

More information

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

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

TSBB09 Image Sensors 2018-HT2. Image Formation Part 1

TSBB09 Image Sensors 2018-HT2. Image Formation Part 1 TSBB09 Image Sensors 2018-HT2 Image Formation Part 1 Basic physics Electromagnetic radiation consists of electromagnetic waves With energy That propagate through space The waves consist of transversal

More information

Introductions to aberrations OPTI 517

Introductions 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 information

Calibration of AO Systems

Calibration of AO Systems Calibration of AO Systems Application to NAOS-CONICA and future «Planet Finder» systems T. Fusco, A. Blanc, G. Rousset Workshop Pueo Nu, may 2003 Département d Optique Théorique et Appliquée ONERA, Châtillon

More information

OPTICAL IMAGE FORMATION

OPTICAL IMAGE FORMATION GEOMETRICAL IMAGING First-order image is perfect object (input) scaled (by magnification) version of object optical system magnification = image distance/object distance no blurring object distance image

More information

Is Aberration-Free Correction the Best Goal

Is Aberration-Free Correction the Best Goal Is Aberration-Free Correction the Best Goal Stephen Burns, PhD, Jamie McLellan, Ph.D., Susana Marcos, Ph.D. The Schepens Eye Research Institute. Schepens Eye Research Institute, an affiliate of Harvard

More information

Optical transfer function shaping and depth of focus by using a phase only filter

Optical transfer function shaping and depth of focus by using a phase only filter Optical transfer function shaping and depth of focus by using a phase only filter Dina Elkind, Zeev Zalevsky, Uriel Levy, and David Mendlovic The design of a desired optical transfer function OTF is a

More information

Astronomical Observing Techniques Lecture 6: Op:cs

Astronomical Observing Techniques Lecture 6: Op:cs Astronomical Observing Techniques Lecture 6: Op:cs Christoph U. Keller keller@strw.leidenuniv.nl Outline 1. Geometrical Op

More information

Aberrations and adaptive optics for biomedical microscopes

Aberrations and adaptive optics for biomedical microscopes Aberrations and adaptive optics for biomedical microscopes Martin Booth Department of Engineering Science And Centre for Neural Circuits and Behaviour University of Oxford Outline Rays, wave fronts and

More information

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS. GUI Simulation Diffraction: Focused Beams and Resolution for a lens system

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS. GUI Simulation Diffraction: Focused Beams and Resolution for a lens system DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS GUI Simulation Diffraction: Focused Beams and Resolution for a lens system Ian Cooper School of Physics University of Sydney ian.cooper@sydney.edu.au DOWNLOAD

More information

Ocular Shack-Hartmann sensor resolution. Dan Neal Dan Topa James Copland

Ocular Shack-Hartmann sensor resolution. Dan Neal Dan Topa James Copland Ocular Shack-Hartmann sensor resolution Dan Neal Dan Topa James Copland Outline Introduction Shack-Hartmann wavefront sensors Performance parameters Reconstructors Resolution effects Spot degradation Accuracy

More information

Lecture 5. Telescopes (part II) and Detectors

Lecture 5. Telescopes (part II) and Detectors Lecture 5 Telescopes (part II) and Detectors Please take a moment to remember the crew of STS-107, the space shuttle Columbia, as well as their families. Crew of the Space Shuttle Columbia Lost February

More information

A tutorial for designing. fundamental imaging systems

A tutorial for designing. fundamental imaging systems A tutorial for designing fundamental imaging systems OPTI 521 College of Optical Science University of Arizona November 2009 Abstract This tutorial shows what to do when we design opto-mechanical system

More information

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

Lecture 4: Geometrical Optics 2. Optical Systems. Images and Pupils. Rays. Wavefronts. Aberrations. Outline Lecture 4: Geometrical Optics 2 Outline 1 Optical Systems 2 Images and Pupils 3 Rays 4 Wavefronts 5 Aberrations Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl Lecture 4: Geometrical

More information

Tutorial Zemax Introduction 1

Tutorial Zemax Introduction 1 Tutorial Zemax Introduction 1 2012-07-17 1 Introduction 1 1.1 Exercise 1-1: Stair-mirror-setup... 1 1.2 Exercise 1-2: Symmetrical 4f-system... 5 1 Introduction 1.1 Exercise 1-1: Stair-mirror-setup Setup

More information

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

Why 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 information

Optical Design Forms for DUV&VUV Microlithographic Processes

Optical Design Forms for DUV&VUV Microlithographic Processes Optical Design Forms for DUV&VUV Microlithographic Processes James Webb, Julie Bentley, Paul Michaloski, Anthony Phillips, Ted Tienvieri Tropel Corporation, 60 O Connor Road, Fairport, NY 14450 USA, jwebb@tropel.com

More information

Basic Wavefront Aberration Theory for Optical Metrology

Basic Wavefront Aberration Theory for Optical Metrology APPLIED OPTICS AND OPTICAL ENGINEERING, VOL. Xl CHAPTER 1 Basic Wavefront Aberration Theory for Optical Metrology JAMES C. WYANT Optical Sciences Center, University of Arizona and WYKO Corporation, Tucson,

More information

Typical 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 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 information

Solution of Exercises Lecture Optical design with Zemax Part 6

Solution 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

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

Lecture 3: Geometrical Optics 1. Spherical Waves. From Waves to Rays. Lenses. Chromatic Aberrations. Mirrors. Outline Lecture 3: Geometrical Optics 1 Outline 1 Spherical Waves 2 From Waves to Rays 3 Lenses 4 Chromatic Aberrations 5 Mirrors Christoph U. Keller, Leiden Observatory, keller@strw.leidenuniv.nl Lecture 3: Geometrical

More information

INTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS

INTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS INTRODUCTION TO ABERRATIONS IN OPTICAL IMAGING SYSTEMS The competent and intelligent optical design of today s state-of-the-art products requires an understanding of optical aberrations. This accessible

More information

BIG PIXELS VS. SMALL PIXELS THE OPTICAL BOTTLENECK. Gregory Hollows Edmund Optics

BIG PIXELS VS. SMALL PIXELS THE OPTICAL BOTTLENECK. Gregory Hollows Edmund Optics BIG PIXELS VS. SMALL PIXELS THE OPTICAL BOTTLENECK Gregory Hollows Edmund Optics 1 IT ALL STARTS WITH THE SENSOR We have to begin with sensor technology to understand the road map Resolution will continue

More information

There is a range of distances over which objects will be in focus; this is called the depth of field of the lens. Objects closer or farther are

There is a range of distances over which objects will be in focus; this is called the depth of field of the lens. Objects closer or farther are Chapter 25 Optical Instruments Some Topics in Chapter 25 Cameras The Human Eye; Corrective Lenses Magnifying Glass Telescopes Compound Microscope Aberrations of Lenses and Mirrors Limits of Resolution

More information

Vocabulary: Description: Materials: Objectives: Safety: Two 45-minute class periods (one for background and one for activity) Schedule:

Vocabulary: Description: Materials: Objectives: Safety: Two 45-minute class periods (one for background and one for activity) Schedule: Resolution Not just for the New Year Author(s): Alia Jackson Date Created: 07/31/2013 Subject: Physics Grade Level: 11-12 Standards: Standard 1: M1.1 Use algebraic and geometric representations to describe

More information