Freeform metrology using subaperture stitching interferometry

Size: px
Start display at page:

Download "Freeform metrology using subaperture stitching interferometry"

Transcription

1 Freeform metrology using subaperture stitching interferometry APOMA November 10-11, 2016 Presented By: Christopher Hall QED Optics Sr. Engineer, QED Technologies Copyright QED Technologies 2016

2 Interferometry Without Nulls - SSI Key benefits of sub-aperture metrology: Magnify Locally null Higher resolution resolves more fringes QED Algorithms Enable automation Compensate for systematic errors Motion Reference wave Re-trace SSI-A 2 Copyright QED Technologies 2016

3 Subaperture Stitching Interferometry for Freeform Two new developments QIS: QED Interferometer optimized for Stitching Algorithms extended to freeform geometries QIS Enables capture of higher fringe densities New Algorithms From rotationally symmetric only freeform shapes New motion equations & other algorithm extensions Maintains all the benefits of stitching parts with rotational symmetry (reference wave calibration, distortion calibration, etc.) Still under development 3 Copyright QED Technologies 2016

4 Subaperture Stitching Interferometry Interferometry can typically provide higher lateral resolution and precision than CMM metrology or profilometry ASI platform excels at measuring mid-spatial frequency errors Extended some aspects of our stitching algorithms to support nonrotationally symmetric geometries Freeform geometry input Freeform motion equations Still more work to be done Using a 4 f/7.2, a 5 mm subaperture patch could be measured ~16 µm freeform departure over 5 mm Φ 166 sub-aps collect to cover 28 mm Φ area; ~600 µm freeform departure 4 Copyright QED Technologies 2016

5 Subaperture Stitching Interferometry Results Low order error agrees very well Greatly increased resolution over CMM 1200 pix (SSI) vs 60 pix (CMM) 23 µm/pix vs 460 µm/pix Mid-spatial frequencies are characterized much more clearly by SSI Vertical trough is clearly seen in SSI measurement, but barely visible in CMM measurement Horizontal ripples have higher definition For high precision figure correction, both CMM and SSI measurements are valuable SSI Color Scale +/- 40 µm POW & alignment errors removed Color Scale +/ µm 4 mm high-pass filter CMM Vertical trough seen by SSI but not by CMM 28 mm 26 mm 5 Copyright QED Technologies 2016

6 Freeform telescope mirror Dominant terms in Q-polynomial freeform representation: Q 0 2 = 66 µm (astigmatism-like) Q 1 1 = 50 µm (coma-like) Q 0 0 = 21 µm (spherical-like) Q 0 3 = 20 µm (trefoil-like) 106 μm PV departure from best-fit sphere 6 Copyright QED Technologies 2016

7 Metrology of telescope mirror CGH vs SSI For CGH: 4 interferometer on horizontal table 4 f/1.5 TS ~600 x 600 pixels For Stitching: ASI(Q) Interferometer 6 f/3.5 TS 47 Subapertures ~2K x 2K pixels Lattice Design All data reported over 100 mm clear aperture 7 Copyright QED Technologies 2016

8 ASI Repeatability Three repeat measurements RMS: 78 nm RMS: 77 nm RMS: 76 nm Pixel-by-pixel mean and standard deviation ASI(Q) gives very repeatable measurements RMS: 77 nm RMS: 2 nm 8 Copyright QED Technologies 2016

9 Comparison with CGH Metrology Difficulty of measurement execution Lateral resolution Mid-spatial frequency characterization Distortion 9 Copyright QED Technologies 2016

10 Comparison with CGH metrology CGH Null ASI(Q) Freeform stitching PV = 518 nm RMS = 77 nm PV = 527 nm RMS = 77 nm Results agree very closely >10x more pixels (250,000 vs 3,000,000) 10 Copyright QED Technologies 2016 ASI(Q) gives very good low-order accuracy

11 ASI measurement is easier to execute Software-assisted alignment (initial setup takes minutes instead of hours) Automatic subaperture positioning Easy-to-use data analysis tools Actual fringes Expected fringes 11 Copyright QED Technologies 2016

12 ASI measurement is easier to analyze Automatic removal of alignment error On a freeform, can t remove Zernikes like you can for a sphere or asphere (no 1-1 relationship between alignment errors & Zernikes) X shift: Z1, Z5, and Z6 (X tilt, Y primary astigmatism, and X primary coma), Y shift: Z2, Z4, and Z7 (Y tilt, X primary astigmatism, and Y primary coma), and Rotation: Z5, Z6, and Z9 (Y primary astigmatism, X primary coma, and X trefoil). Instead, figure error due to rigid-body alignment errors are removed Rigid-body alignment error removal Zernike removal Difference RMS: 77 nm RMS: 35 nm RMS: 72 nm If Zernike removal is performed instead of a rigid-body fit, some figure error will be mistakenly attributed to alignment error. 12 Copyright QED Technologies 2016

13 ASI gives higher resolution metrology PSD Data of central subaperture Red curve = CGH data Green curve = ASI(Q) data CGH data appears to have higher level of MSF, but ASI(Q) data shows result is actually quite smooth at this level 13 Copyright QED Technologies 2016

14 ASI gives better MSF fidelity Hotspots from higherorder diffraction visible in CGH data Again, CGH data has MSF information that is not actually true surface shape information 14 Copyright QED Technologies 2016

15 ASI gives better MSF fidelity Ripple from ghost fringes ASI(Q) Freeform Stitching has accurate low-order information, and has more high-frequency information and accuracy at the same time 15 Copyright QED Technologies 2016

16 ASI gives distortion-free measurement ASI distortion free +Y -Y In ASI measurements, rings are at the same radial position at +Y and -Y CGH Up to 1.2mm lateral error In CGH measurements, distortion causes rings to appear at different distances from the center, making a deterministic correction of these features impossible 16 Copyright QED Technologies 2016

17 Correction with MRF Initial After MRF 7x rms improvement demonstrates high convergence as a result of reproducible metrology 17 Copyright QED Technologies 2016

18 Summary ASI(Q) Freeform Stitching is bringing high accuracy and high resolution to full 3-D freeform metrology Critical for deterministic figure and MSF correction using processes like MRF Freeform measurements are very repeatable and show very good agreement with CGH cross-tests Several benefits of ASI measurement over CGH Easier measurement execution Improved lateral resolution Better fidelity of mid-spatial frequency (MSF) features Distortion-free measurement 18 Copyright QED Technologies 2016

SWING ARM OPTICAL CMM

SWING ARM OPTICAL CMM SWING ARM OPTICAL CMM Peng Su, Chang Jin Oh, Robert E. Parks, James H. Burge College of Optical Sciences University of Arizona, Tucson, AZ 85721 OVERVIEW The swing arm profilometer described in reference

More information

Freeform Monolithic Multi-Surface Telescope Manufacturing NASA Mirror Tech Days 1 November 2016

Freeform Monolithic Multi-Surface Telescope Manufacturing NASA Mirror Tech Days 1 November 2016 Freeform Monolithic Multi-Surface Telescope Manufacturing NASA Mirror Tech Days 1 November 2016 Presented By: Joey Lawson, PhD., Todd Blalock Presented By: Freeform Optics Overview Freeforms: Optics that

More information

Fabrication of Freeform Optics

Fabrication of Freeform Optics Fabrication of Freeform Optics Todd Blalock, Kate Medicus, Jessica DeGroote Nelson Optimax Systems, Inc., 6367 Dean Parkway, Ontario, NY 14519 ABSTRACT Freeform surfaces on optical components have become

More information

Freeform grinding and polishing with PROSurf

Freeform grinding and polishing with PROSurf Freeform grinding and polishing with PROSurf Franciscus Wolfs, Edward Fess, Scott DeFisher, Josh Torres, James Ross OptiPro Systems, 6368 Dean Parkway, Ontario, NY 14519 ABSTRACT Recently, the desire to

More information

OPTI 513R / Optical Testing

OPTI 513R / Optical Testing OPTI 513R / Optical Testing Instructor: Dae Wook Kim Meinel Building Rm 633, University of Arizona, Tucson, AZ 85721 E-Mail: dkim@optics.arizona.edu Website: sites.google.com/site/opti513r/ Office Hours:

More information

PROCEEDINGS OF SPIE. Model-free optical surface reconstruction from deflectometry data. L. R. Graves, H. Choi, W. Zhao, C. J. Oh, P. Su, et al.

PROCEEDINGS OF SPIE. Model-free optical surface reconstruction from deflectometry data. L. R. Graves, H. Choi, W. Zhao, C. J. Oh, P. Su, et al. PROCEEDINGS OF SPIE SPIEDigitalLibrary.org/conference-proceedings-of-spie Model-free optical surface reconstruction from deflectometry data L. R. Graves, H. Choi, W. Zhao, C. J. Oh, P. Su, et al. L. R.

More information

Null test for a highly paraboloidal mirror

Null test for a highly paraboloidal mirror Null test for a highly paraboloidal mirror Taehee Kim, James H. Burge, Yunwoo Lee, and Sungsik Kim A circular null computer-generated hologram CGH was used to test a highly paraboloidal mirror diameter,

More information

ABSTRACT 1. INTRODUCTION

ABSTRACT 1. INTRODUCTION The Use of Diffractive Imitator Optics as Calibration Artefacts Paul C T Rees *a, John B. Mitchell a, Andy Volkov a, Jean-Michel Asfour b, Frank Weidner b, Alexander G. Poleshchuk c, Ruslan K. Nasyrov

More information

Who s afraid of freeform optics? * Webinar 17 January 2018

Who s afraid of freeform optics? * Webinar 17 January 2018 Who s afraid of freeform optics? * Webinar 17 January 2018 Outline About the presenters Spectrum Scientific, Inc. (SSI) Challenges of using freeform optics How to use freeform optics Low cost replicas

More information

REPORT DOCUMENTATION PAGE

REPORT DOCUMENTATION PAGE REPORT DOCUMENTATION PAGE Form Approved OMB No. 74-188 Public reporting burden for this collection of information is estimated to average 1 hour per response, including the time for reviewing instructions,

More information

9.0 Special Interferometric Tests for Aspherical Surfaces

9.0 Special Interferometric Tests for Aspherical Surfaces 9.0 Special Interferometric Tests for Aspherical Surfaces 9.0 Special Interferometric Tests for Aspherical Surfaces - I n 9.1 Aspheric Surfaces 9.1.1 Conic 9.1.2 Sag for Aspheres n 9.2 Null Test 9.2.1

More information

Calibration of a portable interferometer for fiber optic connector endface measurements

Calibration of a portable interferometer for fiber optic connector endface measurements Calibration of a portable interferometer for fiber optic connector endface measurements E. Lindmark Ph.D Light Source Reference Mirror Beamsplitter Camera Calibrated parameters Interferometer Interferometer

More information

Freeform polishing with UltraForm finishing

Freeform polishing with UltraForm finishing Freeform polishing with UltraForm finishing Franciscus Wolfs, Edward Fess, Scott DeFisher OptiPro Systems, 6368 Dean Parkway, Ontario, NY 14519 ABSTRACT Recently, the desire to use freeform optics has

More information

Determination and compensation of the reference surface from redundant sets of surface measurements

Determination and compensation of the reference surface from redundant sets of surface measurements Determination and compensation of the reference surface from redundant sets of surface measurements François Polack and Muriel Thomasset Synchrotron SOLEIL, Saint-Aubin, FRANCE IWXM 4, Barcelona July 212

More information

Measurement of Highly Parabolic Mirror using Computer Generated Hologram

Measurement of Highly Parabolic Mirror using Computer Generated Hologram Measurement of Highly Parabolic Mirror using Computer Generated Hologram Taehee Kim a, James H. Burge b, Yunwoo Lee c a Digital Media R&D Center, SAMSUNG Electronics Co., Ltd., Suwon city, Kyungki-do,

More information

Tilted Wave Interferometer Improved Measurement Uncertainty. Germany. ABSTRACT

Tilted Wave Interferometer Improved Measurement Uncertainty. Germany. ABSTRACT URN (Paper): urn:nbn:de:gbv:ilm1-2014iwk-118:5 58 th ILMENAU SCIENTIFIC COLLOQUIUM Technische Universität Ilmenau, 08 12 September 2014 URN: urn:nbn:gbv:ilm1-2014iwk:3 Tilted Wave Interferometer Improved

More information

Optical Characterization of Complex Freeform Surfaces

Optical Characterization of Complex Freeform Surfaces Optical Characterization of Complex Freeform Surfaces By: Scott DeFisher, Ed Fess NASA SBIR Phase I NASA Mirror Tech Days Open Session November 19, 2014 Overview Phase I Summary Goals and Specifications

More information

Ping Zhou. Copyright Ping Zhou A Dissertation Submitted to the Faculty of the. In Partial Fulfillment of the Requirements For the Degree of

Ping Zhou. Copyright Ping Zhou A Dissertation Submitted to the Faculty of the. In Partial Fulfillment of the Requirements For the Degree of ERROR ANALYSIS AND DATA REDUCTION FOR INTERFEROMETRIC SURFACE MEASUREMENTS by Ping Zhou Copyright Ping Zhou 29 A Dissertation Submitted to the Faculty of the COLLEGE OF OPTICAL SCIENCES In Partial Fulfillment

More information

Invited Paper. Katherine Creath and James C. Wyant WYKO Corporation 2650 East Elvira Road, Tucson, Arizona ABSTRACT 1. INTRODUCTION.

Invited Paper. Katherine Creath and James C. Wyant WYKO Corporation 2650 East Elvira Road, Tucson, Arizona ABSTRACT 1. INTRODUCTION. Invited Paper Absolute Measurement of Spherical Surfaces Katherine Creath and James C. Wyant WYKO Corporation 2650 East Elvira Road, Tucson, Arizona 85706 ABSTRACT The testing of spherical surfaces using

More information

Keywords: Random ball test, interferometer calibration, diffraction, retrace, imaging distortion

Keywords: Random ball test, interferometer calibration, diffraction, retrace, imaging distortion Limits for interferometer calibration using the random ball test Ping Zhou*, James H. Burge College of Optical Science, Univ. of Arizona, 63 E. Univ. Blvd, Tucson, AZ, USA 857 ABSTRACT The random ball

More information

Testing spherical surfaces: a fast, quasi-absolute technique

Testing spherical surfaces: a fast, quasi-absolute technique Testing spherical surfaces: a fast, quasi-absolute technique Katherine Creath and James C. Wyant A technique for measuring the quality of spherical surfaces that provides a quasi-absolute result is presented.

More information

Integrated Ray Tracing (IRT) simulation of SCOTS surface measurement of GMT Fast Steering Mirror Prototype

Integrated Ray Tracing (IRT) simulation of SCOTS surface measurement of GMT Fast Steering Mirror Prototype Integrated Ray Tracing (IRT) simulation of SCOTS surface measurement of GMT Fast Steering Mirror Prototype Ji Nyeong Choi *a,b, Dongok Ryu a,b, Sug-Whan Kim a,b,c, Logan Graves d, Peng Su d, Run Huang

More information

AN OVERVIEW OF FREEFORM OPTICS PRODUCTION Nelson E. Claytor, Donald M. Combs, Oscar M. Lechuga, John J. Mader, Jay Udayasankaran

AN OVERVIEW OF FREEFORM OPTICS PRODUCTION Nelson E. Claytor, Donald M. Combs, Oscar M. Lechuga, John J. Mader, Jay Udayasankaran AN OVERVIEW OF FREEFORM OPTICS PRODUCTION Nelson E. Claytor, Donald M. Combs, Oscar M. Lechuga, John J. Mader, Jay Udayasankaran Fresnel Technologies, Inc., 101 W. Morningside Drive, Fort Worth, TX 76110

More information

DESIGN AND ANALYSIS OF DIFFRACTIVE ASPHERIC NULLS

DESIGN AND ANALYSIS OF DIFFRACTIVE ASPHERIC NULLS DESIGN AND ANALYSIS OF DIFFRACTIVE ASPHERIC NULLS Steven M. Arnold Diffraction International, Minnetonka, MN Diffraction International has developed a general methodology for designing diffractive aspheric

More information

Fundamental Optics for DVD Pickups. The theory of the geometrical aberration and diffraction limits are introduced for

Fundamental Optics for DVD Pickups. The theory of the geometrical aberration and diffraction limits are introduced for Chapter Fundamental Optics for DVD Pickups.1 Introduction to basic optics The theory of the geometrical aberration and diffraction limits are introduced for estimating the focused laser beam spot of a

More information

Efficient wave-optical calculation of 'bad systems'

Efficient wave-optical calculation of 'bad systems' 1 Efficient wave-optical calculation of 'bad systems' Norman G. Worku, 2 Prof. Herbert Gross 1,2 25.11.2016 (1) Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany (2)

More information

Imaging Freeform Optical Systems Designed with NURBS Surfaces

Imaging Freeform Optical Systems Designed with NURBS Surfaces Imaging Freeform Optical Systems Designed with NURBS Surfaces Michael P. Chrisp, a Brian Primeau, a Michael A. Echter, ab a MIT Lincoln Laboratory, 244 Wood Street, Lexington, MA, USA 02420 b University

More information

WORCESTER POLYTECHNIC INSTITUTE

WORCESTER POLYTECHNIC INSTITUTE WORCESTER POLYTECHNIC INSTITUTE MECHANICAL ENGINEERING DEPARTMENT Optical Metrology and NDT ME-593L, C 2018 Introduction: Wave Optics January 2018 Wave optics: coherence Temporal coherence Review interference

More information

Baseline Shack Hartmann Design for the 6.5m MMT f/9 Focus

Baseline Shack Hartmann Design for the 6.5m MMT f/9 Focus Baseline Shack Hartmann Design for the 6.5m MMT f/9 Focus S. C. West (swest@as.arizona.edu) and H. Olson 1 Multiple Mirror Telescope Observatory, Tucson, AZ MMTO Technical Memo #01-01, September 2001 http://nemo.as.arizona.edu/~swest/pdfs/sh_wfs_tb.pdf

More information

Software Reference Manual June, 2015 revision 3.1

Software Reference Manual June, 2015 revision 3.1 Software Reference Manual June, 2015 revision 3.1 Innovations Foresight 2015 Powered by Alcor System 1 For any improvement and suggestions, please contact customerservice@innovationsforesight.com Some

More information

How to Measure Wedge. Purpose. Introduction. Tools Needed

How to Measure Wedge. Purpose. Introduction. Tools Needed Purpose Optical Wedge Application (OWA) is an add-on analysis tool for measurement of optical wedges in either transmission or reflection. OWA can measure a single part or many parts simultaneously (e.g.

More information

A RADIAL WHITE LIGHT INTERFEROMETER FOR MEASUREMENT OF CYLINDRICAL GEOMETRIES

A RADIAL WHITE LIGHT INTERFEROMETER FOR MEASUREMENT OF CYLINDRICAL GEOMETRIES A RADIAL WHITE LIGHT INTERFEROMETER FOR MEASUREMENT OF CYLINDRICAL GEOMETRIES Andre R. Sousa 1 ; Armando Albertazzi 2 ; Alex Dal Pont 3 CEFET/SC Federal Center for Technological Education of Sta. Catarina

More information

Lens Design I. Lecture 1: Basics Herbert Gross. Summer term

Lens Design I. Lecture 1: Basics Herbert Gross. Summer term Lens Design I Lecture 1: Basics 2015-04-04 Herbert Gross Summer term 2016 www.iap.uni-jena.de 2 Preliminary Schedule 1 04.04. Basics 2 11.04. Properties of optical systems I 3 18.04. 4 25.04. Properties

More information

Use of the surface PSD and incident angle adjustments to investigate near specular scatter from smooth surfaces

Use of the surface PSD and incident angle adjustments to investigate near specular scatter from smooth surfaces Use of the surface PSD and incident angle adjustments to investigate near specular scatter from smooth surfaces Kashmira Tayabaly a, John C. Stover b, Robert E. Parks a,c, Matthew Dubin a, James H. Burge*

More information

Final Exam. Today s Review of Optics Polarization Reflection and transmission Linear and circular polarization Stokes parameters/jones calculus

Final Exam. Today s Review of Optics Polarization Reflection and transmission Linear and circular polarization Stokes parameters/jones calculus Physics 42200 Waves & Oscillations Lecture 40 Review Spring 206 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 2 You can bring one double-sided pages of notes/formulas.

More information

Internal Tilt-Compensated Coma-Free Decenter of the AXAF mirrors

Internal Tilt-Compensated Coma-Free Decenter of the AXAF mirrors Chapter 30 Internal Tilt-Compensated Coma-Free Decenter of the AXAF mirrors Terrance J. Gaetz This chapter discusses the investigation and analysis of one of the major minor mysteries encountered during

More information

Waves & Oscillations

Waves & Oscillations Physics 42200 Waves & Oscillations Lecture 40 Review Spring 2016 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 112 You can bring one double-sided pages of notes/formulas.

More information

SIMULATION AND VISUALIZATION IN THE EDUCATION OF COHERENT OPTICS

SIMULATION AND VISUALIZATION IN THE EDUCATION OF COHERENT OPTICS SIMULATION AND VISUALIZATION IN THE EDUCATION OF COHERENT OPTICS J. KORNIS, P. PACHER Department of Physics Technical University of Budapest H-1111 Budafoki út 8., Hungary e-mail: kornis@phy.bme.hu, pacher@phy.bme.hu

More information

COMPARISON OF TWO INSTRUMENT DESIGNS FOR NON-CONTACT MEASUREMENT OF GOSSAMER MIRRORS

COMPARISON OF TWO INSTRUMENT DESIGNS FOR NON-CONTACT MEASUREMENT OF GOSSAMER MIRRORS COMPARISON OF TWO INSTRUMENT DESIGNS FOR NON-CONTACT MEASUREMENT OF GOSSAMER MIRRORS Phil Smith and R. Ryan Vallance Precision Systems Laboratory, University of Kentucky * Abstract Lightweight, large format

More information

Metrology for Characterization of Wafer Thickness Uniformity During 3D-IC Processing. SEMATECH Workshop on 3D Interconnect Metrology

Metrology for Characterization of Wafer Thickness Uniformity During 3D-IC Processing. SEMATECH Workshop on 3D Interconnect Metrology Metrology for Characterization of Wafer Thickness Uniformity During 3D-IC Processing SEMATECH Workshop on 3D Interconnect Metrology Chris Lee July 11, 2012 Outline Introduction Motivation For New Metrology

More information

Waves & Oscillations

Waves & Oscillations Physics 42200 Waves & Oscillations Lecture 41 Review Spring 2013 Semester Matthew Jones Final Exam Date:Tuesday, April 30 th Time:1:00 to 3:00 pm Room: Phys 112 You can bring two double-sided pages of

More information

(Goal 3) (Goal 3) (Goals 4 and 5) (Goals 4 and 5)

(Goal 3)  (Goal 3) (Goals 4 and 5) (Goals 4 and 5) 10 This thesis addresses the measurement of geometrical properties (surface geometry, tilt and decentration) of the crystalline lens in normal eyes, and their changes with accommodation. In addition, it

More information

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 3: Properties of optical systems II 205-04-27 Herbert Gross Summer term 205 www.iap.uni-jena.de 2 Preliminary Schedule 3.04. Basics 2 20.04. Properties of optical systems I 3 27.05.

More information

High Performance, Full-Digital Control on the LMT and KVN Telescopes

High Performance, Full-Digital Control on the LMT and KVN Telescopes High Performance, Full-Digital Control on the LMT and KVN Telescopes David R. Smith (MERLAB), alpha@merlab.com Kamal Souccar (UMass), David Gale (INAOE), F. Peter Schloerb (Umass), David Hughes (INAOE)

More information

Contrast Optimization: A faster and better technique for optimizing on MTF ABSTRACT Keywords: INTRODUCTION THEORY

Contrast Optimization: A faster and better technique for optimizing on MTF ABSTRACT Keywords: INTRODUCTION THEORY Contrast Optimization: A faster and better technique for optimizing on MTF Ken Moore, Erin Elliott, Mark Nicholson, Chris Normanshire, Shawn Gay, Jade Aiona Zemax, LLC ABSTRACT Our new Contrast Optimization

More information

Tolerance on material inhomogenity and surface irregularity

Tolerance on material inhomogenity and surface irregularity Opti 521 Wenrui Cai Tolerance on material inhomogenity and surface irregularity Abstract In this tutorial, a case study on tolerance for a focusing doublet is performed by using ZEMAX. First, how to perform

More information

Hyperspectral interferometry for single-shot absolute measurement of 3-D shape and displacement fields

Hyperspectral interferometry for single-shot absolute measurement of 3-D shape and displacement fields EPJ Web of Conferences 6, 6 10007 (2010) DOI:10.1051/epjconf/20100610007 Owned by the authors, published by EDP Sciences, 2010 Hyperspectral interferometry for single-shot absolute measurement of 3-D shape

More information

Optical Design with Zemax

Optical Design with Zemax Optical Design with Zemax Lecture 7: Optimization I 2012-12-11 Herbert Gross Winter term 2012 www.iap.uni-jena.de Time schedule 2 1 16.10. Introduction Introduction, Zemax interface, menues, file handling,

More information

Meet Your Augmented and Virtual Reality Challenges Head-On: Design Your Next System with 2D-Q Freeforms in CODE V

Meet Your Augmented and Virtual Reality Challenges Head-On: Design Your Next System with 2D-Q Freeforms in CODE V WHITE PAPER Meet Your Augmented and Virtual Reality Challenges Head-On: Design Your Next System with 2D-Q Freeforms in CODE V Author Matt Novak, Ph.D. CODE V Sr. Customer Applications Engineer, Synopsys

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION doi:10.1038/nature10934 Supplementary Methods Mathematical implementation of the EST method. The EST method begins with padding each projection with zeros (that is, embedding

More information

Iterative procedure for in-situ EUV optical testing with an incoherent source

Iterative procedure for in-situ EUV optical testing with an incoherent source APS/123-QED Iterative procedure for in-situ EUV optical testing with an incoherent source Ryan Miyakawa and Patrick Naulleau Lawrence Berkeley National Laboratory, Berkeley, CA 94720 Avideh Zakhor Dept.

More information

Lens Design I. Lecture 11: Imaging Herbert Gross. Summer term

Lens Design I. Lecture 11: Imaging Herbert Gross. Summer term Lens Design I Lecture 11: Imaging 2015-06-29 Herbert Gross Summer term 2015 www.iap.uni-jena.de 2 Preliminary Schedule 1 13.04. Basics 2 20.04. Properties of optical systrems I 3 27.05. 4 04.05. Properties

More information

3.6 Rotational-Shearing Interferometry for Improved Target Characterization

3.6 Rotational-Shearing Interferometry for Improved Target Characterization 3.6 Rotational-Shearing Interferometry for Improved Target Characterization Inertial-fusion targets have strict requirements regarding sphericity, surface smoothness, and layer-thickness uniformity. During

More information

ARL OESIADAU INNOVATIONS

ARL OESIADAU INNOVATIONS ARL OESIADAU INNOVATIONS About Us Contacts Opto-Mechanical Design Precision OPtical Polishing Surface metrology Case Studies About Us Ltd is a technology company, located in the OpTIC Centre, a large scale

More information

A method of evaluating and tolerancing interferometer designs

A method of evaluating and tolerancing interferometer designs A method of evaluating and tolerancing interferometer designs Paul Michaloski, Andrew Kulawiec, Jon Fleig Tropel Corporation 6 O'Connor Road Fairport, New York 1445 Abstract A ray tracing method of simulating

More information

Precision Engineering

Precision Engineering Precision Engineering 37 (213) 599 65 Contents lists available at SciVerse ScienceDirect Precision Engineering jou rnal h om epage: www.elsevier.com/locate/precision Random error analysis of profile measurement

More information

109-channel 50mm piezoelectric deformable mirror system technical passport

109-channel 50mm piezoelectric deformable mirror system technical passport F L E X I B L E Flexible Optical B.V. Adaptive Optics Optical Microsystems Wavefront Sensors O P T I C A L Oleg Soloviev Chief Scientist Röntgenweg 1 2624 BD, Delft The Netherlands Tel: +31 15 285 15-47

More information

Invited Paper. Telescope. James H. Burge a ABSTRACT M5 M2

Invited Paper. Telescope. James H. Burge a ABSTRACT M5 M2 Invited Paper Alignment of 4-mirror r Wide Field Corrector for the Hobby-Eberly Telescope Chang Jin Oh* a, Eric H. Frater a, Laura Coyle a, Matt Dubin a, Andrew Lowman a, Chunyu Zhao a, James H. Burge

More information

Optimal Support Solution for a Meniscus Mirror Blank

Optimal Support Solution for a Meniscus Mirror Blank Preliminary Design Review Optimal Support Solution for a Meniscus Mirror Blank Opti 523 Independent Project Edgar Madril Scope For this problem an optimal solution for a mirror support is to be found for

More information

Using a multipoint interferometer to measure the orbital angular momentum of light

Using a multipoint interferometer to measure the orbital angular momentum of light CHAPTER 3 Using a multipoint interferometer to measure the orbital angular momentum of light Recently it was shown that the orbital angular momentum of light can be measured using a multipoint interferometer,

More information

Modeling interferometers with lens design software

Modeling interferometers with lens design software Modeling interferometers with lens design software Bryan D. Stone, MEMBER SPIE Tropel Corporation 60 O Connor Road Fairport, ew York 14450 Abstract. Lens design software has been designed primarily to

More information

Lens Design I. Lecture 4: Properties of optical systems III Herbert Gross. Summer term

Lens Design I. Lecture 4: Properties of optical systems III Herbert Gross. Summer term Lens Design I Lecture 4: Properties of optical systems III 018-05-03 Herbert Gross Summer term 018 www.iap.uni-jena.de Preliminary Schedule - Lens Design I 018 1 1.04. Basics 19.04. Properties of optical

More information

Applications of Piezo Actuators for Space Instrument Optical Alignment

Applications of Piezo Actuators for Space Instrument Optical Alignment Year 4 University of Birmingham Presentation Applications of Piezo Actuators for Space Instrument Optical Alignment Michelle Louise Antonik 520689 Supervisor: Prof. B. Swinyard Outline of Presentation

More information

Lens Design. Craig Olson. Julie Bentley. Field Guide to. John E. Greivenkamp, Series Editor SPIE. SPIE Field Guides. Volume FG27

Lens Design. Craig Olson. Julie Bentley. Field Guide to. John E. Greivenkamp, Series Editor SPIE. SPIE Field Guides. Volume FG27 Field Guide to Lens Design Julie Bentley Craig Olson SPIE Field Guides Volume FG27 John E. Greivenkamp, Series Editor SPIE PRESS Bellingham,Washington USA vii Glossary of Symbols and Acronyms xi Fundamentals

More information

OPTI-521 Graduate Report 2 Matthew Risi Tutorial: Introduction to imaging, and estimate of image quality degradation from optical surfaces

OPTI-521 Graduate Report 2 Matthew Risi Tutorial: Introduction to imaging, and estimate of image quality degradation from optical surfaces OPTI-521 Graduate Report 2 Matthew Risi Tutorial: Introduction to imaging, and estimate of image quality degradation from optical surfaces Abstract The purpose of this tutorial is to introduce the concept

More information

On the quality of measured optical aberration coefficients using phase wheel monitor

On the quality of measured optical aberration coefficients using phase wheel monitor On the quality of measured optical aberration coefficients using phase wheel monitor Lena V. Zavyalova *, Aaron R. Robinson, Anatoly Bourov, Neal V. Lafferty, and Bruce W. Smith Center for Nanolithography

More information

Welcome to: Physics I. I m Dr Alex Pettitt, and I ll be your guide!

Welcome to: Physics I. I m Dr Alex Pettitt, and I ll be your guide! Welcome to: Physics I I m Dr Alex Pettitt, and I ll be your guide! Physics I: x Mirrors and lenses Lecture 13: 6-11-2018 Last lecture: Reflection & Refraction Reflection: Light ray hits surface Ray moves

More information

Bonnet Polishing and Fluid Jet Polishing

Bonnet Polishing and Fluid Jet Polishing Bonnet Polishing and Fluid Jet Polishing Zeeko., Ltd. Richard Freeman 1. Introduction 1.1 The need for free-form surfaces The capability of producing free-form surfaces surfaces not limited to regular

More information

Basic optics. Geometrical optics and images Interference Diffraction Diffraction integral. we use simple models that say a lot! more rigorous approach

Basic optics. Geometrical optics and images Interference Diffraction Diffraction integral. we use simple models that say a lot! more rigorous approach Basic optics Geometrical optics and images Interference Diffraction Diffraction integral we use simple models that say a lot! more rigorous approach Basic optics Geometrical optics and images Interference

More information

Stevens High School AP Physics II Work for Not-school

Stevens High School AP Physics II Work for Not-school 1. Gravitational waves are ripples in the fabric of space-time (more on this in the next unit) that travel at the speed of light (c = 3.00 x 10 8 m/s). In 2016, the LIGO (Laser Interferometry Gravitational

More information

Tutorial Zemax 6: Advanced handling

Tutorial Zemax 6: Advanced handling Tutorial Zemax 6: Advanced handling 2012-09-25 6 Advanced handling 1 6.1 Multi configuration, universal plot and slider... 1 6.2 Macro for Spot Moments... 6 6.3 Multiconfiguration and folding mirror...

More information

Cameras and Radiometry. Last lecture in a nutshell. Conversion Euclidean -> Homogenous -> Euclidean. Affine Camera Model. Simplified Camera Models

Cameras and Radiometry. Last lecture in a nutshell. Conversion Euclidean -> Homogenous -> Euclidean. Affine Camera Model. Simplified Camera Models Cameras and Radiometry Last lecture in a nutshell CSE 252A Lecture 5 Conversion Euclidean -> Homogenous -> Euclidean In 2-D Euclidean -> Homogenous: (x, y) -> k (x,y,1) Homogenous -> Euclidean: (x, y,

More information

Rodenstock Products Photo Optics / Digital Imaging

Rodenstock Products Photo Optics / Digital Imaging Go to: Apo-Sironar digital Apo-Macro-Sironar digital Apo-Sironar digital HR Lenses for Digital Professional Photography Digital photography may be superior to conventional photography if the end-product

More information

Ray Optics I. Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex

Ray Optics I. Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex Phys 531 Lecture 8 20 September 2005 Ray Optics I Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex Today shift gears, start applying

More information

College Physics 150. Chapter 25 Interference and Diffraction

College Physics 150. Chapter 25 Interference and Diffraction College Physics 50 Chapter 5 Interference and Diffraction Constructive and Destructive Interference The Michelson Interferometer Thin Films Young s Double Slit Experiment Gratings Diffraction Resolution

More information

ksa MOS Ultra-Scan Performance Test Data

ksa MOS Ultra-Scan Performance Test Data ksa MOS Ultra-Scan Performance Test Data Introduction: ksa MOS Ultra Scan 200mm Patterned Silicon Wafers The ksa MOS Ultra Scan is a flexible, highresolution scanning curvature and tilt-measurement system.

More information

WORCESTER POLYTECHNIC INSTITUTE

WORCESTER POLYTECHNIC INSTITUTE WORCESTER POLYTECHNIC INSTITUTE MECHANICAL ENGINEERING DEPARTMENT Optical Metrology and NDT ME-593L, C 2018 Lecture 03 January 2018 Lasers sources Some operating characteristics: laser modes Schematic

More information

Aberration Theory. Lens. Optical systems convert the shapes of wavefronts

Aberration Theory. Lens. Optical systems convert the shapes of wavefronts Aberration Theory Lens Optical systems convert the shapes of wavefronts Aberrations A perfectly spherical wave will converge to a point. Any deviation from the ideal spherical shape is said to be an aberration.

More information

Novel Magnetic Field Mapping Technology for Small and Closed Aperture Undulators

Novel Magnetic Field Mapping Technology for Small and Closed Aperture Undulators Novel Magnetic Field Mapping Technology for Small and Closed Aperture Undulators Erik Wallen and Hyun-Wook Kim 06.06.2017 Outline Introduction - Measurement systems at LBNL - Activities at LBNL - Need

More information

Southern African Large Telescope. PFIS Distortion and Alignment Model

Southern African Large Telescope. PFIS Distortion and Alignment Model Southern African Large Telescope PFIS Distortion and Alignment Model Kenneth Nordsieck University of Wisconsin Document Number: SALT-3120AS0023 Revision 2.0 31 May 2006 Change History Rev Date Description

More information

Eric Lindmark, Ph.D.

Eric Lindmark, Ph.D. Theory and Practical Application Written by: Eric Lindmark, Ph.D. v061608 4611 Chatsworth Street Shoreview, Minnesota, 55126-5813, USA www.promet.net Introduction In theory, higher bit rate fiber optic

More information

19- channel piezoelectric deformable mirror system technical passport

19- channel piezoelectric deformable mirror system technical passport F L E X I B L E Flexible Optical B.V. Adaptive Optics Optical Microsystems Wavefront Sensors O P T I C A L Oleg Soloviev Chief Scientist Röntgenweg 1 BD, Delft The Netherlands Tel: +1 1 1- Fax: +1 1 1-

More information

ADVANCED TECHNOLOGIES FOR FABRICATION AND TESTING OF LARGE FLAT MIRRORS

ADVANCED TECHNOLOGIES FOR FABRICATION AND TESTING OF LARGE FLAT MIRRORS 1 ADVANCED TECHNOLOGIES FOR FABRICATION AND TESTING OF LARGE FLAT MIRRORS by Julius Eldon Yellowhair Copyright Julius E. Yellowhair 2007 A Dissertation Submitted to the Faculty of the COLLEGE OF OPTICAL

More information

Chapter 3 Image Registration. Chapter 3 Image Registration

Chapter 3 Image Registration. Chapter 3 Image Registration Chapter 3 Image Registration Distributed Algorithms for Introduction (1) Definition: Image Registration Input: 2 images of the same scene but taken from different perspectives Goal: Identify transformation

More information

CleaveMeter TM. Interferometric fiber end-face inspection systems for research, development and production.

CleaveMeter TM.  Interferometric fiber end-face inspection systems for research, development and production. CleaveMeter TM Interferometric fiber end-face inspection systems for research, development and production Product catalogue NYFORS is a trademark of Nyfors Teknologi AB. Edition 2013 January. Interferometric

More information

High-resolution 3D profilometry with binary phase-shifting methods

High-resolution 3D profilometry with binary phase-shifting methods High-resolution 3D profilometry with binary phase-shifting methods Song Zhang Department of Mechanical Engineering, Iowa State University, Ames, Iowa 511, USA (song@iastate.edu) Received 11 November 21;

More information

4D Technology Corporation

4D Technology Corporation 4D Technology Corporation Dynamic Laser Interferometry for Company Profile Disk Shape Characterization DiskCon Asia-Pacific 2006 Chip Ragan chip.ragan@4dtechnology.com www.4dtechnology.com Interferometry

More information

MrFit: Deformable mirror simulator

MrFit: Deformable mirror simulator MrFit: Deformable mirror simulator c Flexible Optical BV (OKO Technologies) Röntgenweg 1, 2624 BD Delft, The Netherlands http://okotech.com February 19, 2008 1 Introduction MrFit is a program for simulation

More information

Metrology and Sensing

Metrology and Sensing Metrology and Sensing Lecture 4: Fringe projection 2016-11-08 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

Quantitative Data Extraction using Spatial Fourier Transform in Inversion Shear Interferometer

Quantitative Data Extraction using Spatial Fourier Transform in Inversion Shear Interferometer Rose-Hulman Institute of Technology Rose-Hulman Scholar Graduate Theses - Physics and Optical Engineering Graduate Theses Summer 8-2014 Quantitative Data Extraction using Spatial Fourier Transform in Inversion

More information

A FEW CASE STUDIES IN UNCERTAINTY USING THE NIST M48 CMM

A FEW CASE STUDIES IN UNCERTAINTY USING THE NIST M48 CMM A FEW CASE STUIES IN UNCERTAINTY USING THE NIST M48 CMM John Stoup Precision Engineering ivision National Institute of Standards and Technology Gaithersburg, Maryland 20899 INTROUCTION The Moore M48 coordinate

More information

PRECISION GEOMETRIC METROLOGY OF REFRACTIVE MICRO-LENSES. Neil William Gardner

PRECISION GEOMETRIC METROLOGY OF REFRACTIVE MICRO-LENSES. Neil William Gardner PRECISION GEOMETRIC METROLOGY OF REFRACTIVE MICRO-LENSES by Neil William Gardner A dissertation submitted to the faculty of The University of North Carolina at Charlotte in partial fulfillment of the requirements

More information

University of Huddersfield Repository

University of Huddersfield Repository University of Huddersfield Repository Li, Duo, Ding, Fei, Jiang, Xiangqian, Blunt, Liam A. and Tong, Zhen Calibration of an interferometric surface measurement system on an ultra precision turning lathe

More information

MEMS SENSOR FOR MEMS METROLOGY

MEMS SENSOR FOR MEMS METROLOGY MEMS SENSOR FOR MEMS METROLOGY IAB Presentation Byungki Kim, H Ali Razavi, F. Levent Degertekin, Thomas R. Kurfess 9/24/24 OUTLINE INTRODUCTION Motivation Contact/Noncontact measurement Optical interferometer

More information

Modeling of diffractive optical elements for lens design.

Modeling of diffractive optical elements for lens design. Juan L. Rayces and Lan Lebich OA Applied Optics, 7421 Orangewood Ave., Garden Grove, A 92641. Abstract. The use of a standard aspheric profile to describe conventional optical elements in lens design programs

More information

Testing of a diamond-turned off-axis parabolic mirror

Testing of a diamond-turned off-axis parabolic mirror Invited Paper Testing of a diamond-turned off-axis parabolic mirror Jan Burke *a, Kai Wang b, Adam Bramble b a CIRO Materials cience and Engineering Australian Centre for Precision Optics, PO Box 218,

More information

USING ARTICULATED METROLOGY ARM TO VERIFY AND ALIGN OPTICAL SURFACES IN TERAHERTZ ASTRONOMY APPLICATIONS

USING ARTICULATED METROLOGY ARM TO VERIFY AND ALIGN OPTICAL SURFACES IN TERAHERTZ ASTRONOMY APPLICATIONS USING ARTICULATED METROLOGY ARM TO VERIFY AND ALIGN OPTICAL SURFACES IN TERAHERTZ ASTRONOMY APPLICATIONS by Mike Borden A Thesis Submitted to the Faculty of the COMMITTEE ON OPTICAL SCIENCES (GRADUATE)

More information

Waves & Oscillations

Waves & Oscillations Physics 42200 Waves & Oscillations Lecture 41 Review Spring 2016 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 112 You can bring one double-sided pages of notes/formulas.

More information

18-channel 50mm piezoelectric deformable mirror system technical passport

18-channel 50mm piezoelectric deformable mirror system technical passport F L E X I B L E Flexible Optical B.V. Adaptive Optics Optical Microsystems Wavefront Sensors O P T I C A L Oleg Soloviev Chief Scientist Röntgenweg 1 BD, Delft The Netherlands Tel: +1 1 1- Fax: +1 1 1-

More information

Exercise 12 Geometrical and Technical Optics WS 2013/2014

Exercise 12 Geometrical and Technical Optics WS 2013/2014 Exercise 12 Geometrical and Technical Optics WS 213/214 Slide projector and Köhler illumination In this exercise a simplified slide projector (or LCD projector) will be designed and simulated with ray

More information