Stereoscopic Hologram

Size: px
Start display at page:

Download "Stereoscopic Hologram"

Transcription

1 Stereoscopic Hologram Joonku Hahn Kyungpook National University

2 Outline: 1. Introduction - Basic structure of holographic display - Wigner distribution function 2. Design of Stereoscopic Hologram - Optical design concept - Viewing window - Spatial light modulator 3. Examples of Stereoscopic Hologram - Holographic display with a large-scale SLM - Projection-type holographic display - Head-mounted holographic display 4. Summary 1

3 1. Introduction Available structure of holographic display Coherent Light Source Optics Electrically addressable Spatial Light Modulator Optical filter Scanner Optically addressable Spatial Light Modulator Optics Screen Observer (optional) (optional) 2

4 1. Introduction Space-bandwidth product N M W W 2 u v u v Data capacity 2 2 Area of image Numerical Aperture wavelength. 2 2 Data capacity Area of screen Field of view wavelength Color depth Space-Bandwidth Product p a p p a p v Spherical phase resulting from d Amplitude contour by sinc function f Pixels of SLM M p W v W u u +1 order diffraction on v-axis Central direction of local viewing angle, c c d Transfer lens N p f Focal plane 0 order diffraction v -1 order diffraction on v-axis u Local viewing angle J. Hahn, H. Kim, Y. Lim, G. Park, and B. Lee, Optics Express 16, pp , (2008). 3

5 1. Introduction Wigner distribution function The area in the Wigner distribution function is equal to the space-bandwidth product. v v v x x x After a Fresnel transform After a Fourier transform A. W. Lohmann, R. G. Dorsch, D. Mendlovic, Z. Zalevsky, and C. Ferreira, J. Opt. Soc. Am. A 13, (1996). 4

6 1. Introduction Definition of the planes in holographic display y v x u Hologram plane Viewing window plane 5

7 1. Introduction Holographic Stereogram vs. Stereoscopic Hologram Hologram plane Viewing window plane Holographic Stereogram Stereoscopic Hologram 6

8 2. Design of Stereoscopic Hologram Stereoscopic Hologram View volume defined by 8K-resolution hologram 40inch 20inch View volume defined by 4K-resolution hologram View volume defined by 2K-resolution hologram 10inch Transverse resolution at screen p 0.11mm Width of viewing window at pupil of eye w 1.8 m p m VW 1.8m 7

9 2. Design of Stereoscopic Hologram Basic geometry of stereoscopic holographic display Viewing window Hologram plane 8

10 2. Design of Stereoscopic Hologram Display with a large-aperture SLM Large-aperture SLM Light source Viewing window Hologram plane 9

11 2. Design of Stereoscopic Hologram Viewing window Spot size of undiffracted light needs to be small enough for fear of disturbing the signal which is modulated by spatial light modulator. 10

12 2. Design of Stereoscopic Hologram Projection-type display Real image Light source Small-aperture SLM Projection optics with a pair of parabolic mirrors Hologram plane Viewing window 11

13 2. Design of Stereoscopic Hologram Types and properties of SLM Full-complex modulation Amplitude-only modulation Im i Im i Re -1 1 Re -1 1 Liquid crystal display (LCD) modulator Digital micro-mirror device (DMD) modulator -i Phase-only modulation -i Typical characteristic of liquid crystal device Im i Im i Re -1 1 Re -1 1 Liquid crystal on Silicon (LCoS) modulator Acousto-optic modulator (AOM) -i -i 12

14 2. Design of Stereoscopic Hologram Off-axis complex hologram encoding with amplitude-only modulation G ( f) 0 G( f) 1 f max (a) fmax f f max (b) fmax f G ( f) 2 G ( f) 3 f max (c) fmax f f max (d) fmax f C.-Y. Hwang, K.-S. Kim, B.-R. Lee, S. Oh, H. Kim, and J. Hahn, Off-axis complex hologram encoding with amplitude-only modulation, Opt. Express submitted. 13

15 2. Design of Stereoscopic Hologram Structure for off-axis complex hologram encoding with amplitude-only modulation y0 y 1 y 2 y 3 y 4 y5 f1 f2 f3 x 0 x 1 x 2 x 3 x 4 x 5 z d1 d2 f1 d3 d4 d5 SLM plane Focal plane Image plane Viewing window plane 14

16 2. Design of Stereoscopic Hologram Head-mount display Virtual image SLM Light source Eyepiece Viewing window Hologram plane 15

17 3. Examples of Stereoscopic Hologram Holographic display with a large-scale SLM Layout Optical design 16

18 3. Examples of Stereoscopic Hologram Holographic display with a large-scale SLM Structure according to functions EYE Tracking Beamsplitter Main Control Large-scale Spatial Light Modulator I/O ports Hologram Calculation Input Optics Array of Point Light Sources 17

19 3. Examples of Stereoscopic Hologram Holographic display with a large-scale SLM Motorized stages with light sources array Input integrated optics Spatial light modulators Control boards Large-format beam splitter xin, yin, zin y xout, yout, zout 182mm 144mm 4.55deg z 500mm 1800mm z=-500mm z=0 z=1800mm 18

20 3. Examples of Stereoscopic Hologram Projection-type holographic display Layout Optical design Viewing windows Holographic display Parabolic mirrors Viewing windows Optics for projection FT lenses SLM Mirrors Light engines 19

21 3. Examples of Stereoscopic Hologram Projection-type holographic display Light engine Left part Mirrors Right part X-cube prism Green Blue Red SLMs X-cube prism Green Collimators SLMs Collimators Laser diode modules Red FT lenses Filters Blue Laser diode modules Polarizer Objective lens Collimation lens Laser diode module Plate spring Pinhole Adjustable tube (a) Red Green Blue 20

22 3. Examples of Stereoscopic Hologram Holographic display with a large-scale SLM 10inch screen 21

23 3. Examples of Stereoscopic Hologram Holographic display with a large-scale SLM Simulation Experiment Focused at the screen Focused 0.9m away from the screen 22

24 3. Examples of Stereoscopic Hologram Head-mounted holographic display Layout Optical design 23

25 3. Examples of Stereoscopic Hologram Head-mounted holographic display Data cable Control box with light sources Holographic display for head-mounted application Multimode optical fiber Multimode optical fiber Beamsplitter at viewing window Control board Red LED Blue LED Green LED Data cable Multimode optical fiber 24

26 x-axis [mm] x-axis [mm] x-axis [mm] 3. Examples of Stereoscopic Hologram x-axis [mm] x-axis [mm] x-axis [mm] x-axis [mm] x-axis [mm] x-axis [mm] Head-mounted holographic display ield on retina Simulation Experiment Complex optical field on retina Complex optical field on retina Complex optical field Red -0.2 (625nm) ield on retina 0.2 Complex optical field on retina 0.2 Complex optical field on retina Complex optical field on retina Green m] -0.2 y-axis [mm] -0.2 y-axis [mm] -0.2 y-axis [mm] (528nm) ield on retina 0.2 Complex optical field on retina 0.2 Complex optical field on retina Complex optical field on retina Blue (462nm) m] -0.2 y-axis [mm] -0.2 y-axis [mm] -0.2 y-axis [mm]

27 4. Summary Stereoscopic hologram has a great potential to display large field through a narrow viewing windows. Optical design of stereoscopic hologram has three possible geometries. The first applies a large-aperture SLM and the second displays a real image of the SLM. The last displays a virtual image of the SLM. We succeeded in constructing several interesting systems under the cooperation with Prof. Kim s group in Korea University. 3 Dimensional Optical Technology I N T E G R A T E D P H O T O N I C D E V I C E S & S Y S T E M S L A B 26

Expanded Exit-Pupil Holographic Head-Mounted Display With High-Speed Digital Micromirror Device

Expanded Exit-Pupil Holographic Head-Mounted Display With High-Speed Digital Micromirror Device ETRI Journal, Volume 40, Number 3, June 2018 366 Expanded Exit-Pupil Holographic Head-Mounted Display With High-Speed Digital Micromirror Device Mugeon Kim, Sungjin Lim, Geunseop Choi, Youngmin Kim, Hwi

More information

LEOK-3 Optics Experiment kit

LEOK-3 Optics Experiment kit LEOK-3 Optics Experiment kit Physical optics, geometrical optics and fourier optics Covering 26 experiments Comprehensive documents Include experiment setups, principles and procedures Cost effective solution

More information

Beam Shaping and Simultaneous Exposure by Diffractive Optical Element in Laser Plastic Welding

Beam Shaping and Simultaneous Exposure by Diffractive Optical Element in Laser Plastic Welding Beam Shaping and Simultaneous Exposure by Diffractive Optical Element in Laser Plastic Welding AKL`12 9th May 2012 Dr. Daniel Vogler Page 1 Motivation: Quality and flexibility diffractive spot shaping

More information

Beam shaping for holographic techniques

Beam shaping for holographic techniques Beam shaping for holographic techniques Alexander Laskin a, Vadim Laskin a, Aleksei Ostrun b a AdlOptica GmbH, Rudower Chaussee 29, 12489 Berlin, Germany b St. Petersburg National Research University of

More information

Optics and Lasers. Matt Young. Including Fibers and Optical Waveguides

Optics and Lasers. Matt Young. Including Fibers and Optical Waveguides Matt Young Optics and Lasers Including Fibers and Optical Waveguides Fourth Revised Edition With 188 Figures Springer-Verlag Berlin Heidelberg New York London Paris Tokyo Hong Kong Barcelona Budapest Contents

More information

Introduction to Optofluidics. 1-5 June Use of spatial light modulators (SLM) for beam shaping and optical tweezers

Introduction to Optofluidics. 1-5 June Use of spatial light modulators (SLM) for beam shaping and optical tweezers 2037-4 Introduction to Optofluidics 1-5 June 2009 Use of spatial light modulators (SLM) for beam shaping and optical tweezers M. Padgett University of Glasgow U.K. Use of spatial light modulators (SLM)

More information

A novel tunable diode laser using volume holographic gratings

A novel tunable diode laser using volume holographic gratings A novel tunable diode laser using volume holographic gratings Christophe Moser *, Lawrence Ho and Frank Havermeyer Ondax, Inc. 85 E. Duarte Road, Monrovia, CA 9116, USA ABSTRACT We have developed a self-aligned

More information

Thin holographic camera with integrated reference distribution

Thin holographic camera with integrated reference distribution Thin holographic camera with integrated reference distribution Joonku Hahn, Daniel L. Marks, Kerkil Choi, Sehoon Lim, and David J. Brady* Department of Electrical and Computer Engineering and The Fitzpatrick

More information

Laser Scanning 3D Display with Dynamic Exit Pupil

Laser Scanning 3D Display with Dynamic Exit Pupil Koç University Laser Scanning 3D Display with Dynamic Exit Pupil Kishore V. C., Erdem Erden and Hakan Urey Dept. of Electrical Engineering, Koç University, Istanbul, Turkey Hadi Baghsiahi, Eero Willman,

More information

4-2 Image Storage Techniques using Photorefractive

4-2 Image Storage Techniques using Photorefractive 4-2 Image Storage Techniques using Photorefractive Effect TAKAYAMA Yoshihisa, ZHANG Jiasen, OKAZAKI Yumi, KODATE Kashiko, and ARUGA Tadashi Optical image storage techniques using the photorefractive effect

More information

Fourier Transformation Hologram Experiment using Liquid Crystal Display. Kenji MISUMI, Yoshikiyo KASHII, Mikio MIMURA (Received September 30, 1999)

Fourier Transformation Hologram Experiment using Liquid Crystal Display. Kenji MISUMI, Yoshikiyo KASHII, Mikio MIMURA (Received September 30, 1999) Mem. Fac. Eng., Osaka City Univ., Vol. 40, pp. 85-91 (1999) Fourier Transformation Hologram Experiment using Liquid Crystal Display Kenji MISUMI, Yoshikiyo KASHII, Mikio MIMURA (Received September 30,

More information

BEAM SHAPING OPTICS TO IMPROVE HOLOGRAPHIC AND INTERFEROMETRIC NANOMANUFACTURING TECHNIQUES Paper N405 ABSTRACT

BEAM SHAPING OPTICS TO IMPROVE HOLOGRAPHIC AND INTERFEROMETRIC NANOMANUFACTURING TECHNIQUES Paper N405 ABSTRACT BEAM SHAPING OPTICS TO IMPROVE HOLOGRAPHIC AND INTERFEROMETRIC NANOMANUFACTURING TECHNIQUES Paper N5 Alexander Laskin, Vadim Laskin AdlOptica GmbH, Rudower Chaussee 9, 89 Berlin, Germany ABSTRACT Abstract

More information

Color electroholography by three colored reference lights simultaneously incident upon one hologram panel

Color electroholography by three colored reference lights simultaneously incident upon one hologram panel Color electroholography by three colored reference lights simultaneously incident upon one hologram panel Tomoyoshi Ito Japan Science and Technology Agency / Department of Medical System Engineering, Chiba

More information

Speckle-free digital holographic recording of a diffusely reflecting object

Speckle-free digital holographic recording of a diffusely reflecting object Speckle-free digital holographic recording of a diffusely reflecting object You Seok Kim, 1 Taegeun Kim, 1,* Sung Soo Woo, 2 Hoonjong Kang, 2 Ting-Chung Poon, 3,4 and Changhe Zhou 4 1 Department of Optical

More information

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name:

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name: EE119 Introduction to Optical Engineering Spring 2002 Final Exam Name: SID: CLOSED BOOK. FOUR 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

Laser Beam Splitting. By Diffractive Optics. Michael A. Golub

Laser Beam Splitting. By Diffractive Optics. Michael A. Golub Laser Beam Splitting By Diffractive Optics Michael A. Golub Recent advances in diffractive optics theory and technology have made beam splitting a valuable resource for optical designers. Programmable,

More information

Study of self-interference incoherent digital holography for the application of retinal imaging

Study of self-interference incoherent digital holography for the application of retinal imaging Study of self-interference incoherent digital holography for the application of retinal imaging Jisoo Hong and Myung K. Kim Department of Physics, University of South Florida, Tampa, FL, US 33620 ABSTRACT

More information

360-degree tabletop electronic holographic display

360-degree tabletop electronic holographic display Vol. 24, No. 22 31 Oct 2016 OPTICS EXPRESS 24999 360-degree tabletop electronic holographic display YONGJUN LIM,1,* KEEHOON HONG,1 HWI KIM,2 HYUN-EUI KIM,1 EUNYOUNG CHANG,1 SOOHYUN LEE,1 TAEONE KIM,1 JEHO

More information

Nanoimprint lithography with a focused laser beam for the fabrication of micro-/nano-hybrid patterns

Nanoimprint lithography with a focused laser beam for the fabrication of micro-/nano-hybrid patterns Supplementary Material (ESI) for Lab on a Chip This journal is The Royal Society of Chemistry 20XX Nanoimprint lithography with a focused laser beam for the fabrication of micro-/nano-hybrid patterns Hyungjun

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

Design of a low-cost, interactive, holographic optical tweezers system

Design of a low-cost, interactive, holographic optical tweezers system Design of a low-cost, interactive, holographic optical tweezers system E. Pleguezuelos, J. Andilla, A. Carnicer, E. Martín-Badosa, S. Vallmitjana and M. Montes-Usategui Universitat de Barcelona, Departament

More information

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name:

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name: EE119 Introduction to Optical Engineering Spring 2003 Final Exam Name: SID: CLOSED BOOK. THREE 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

Large scale rapid access holographic memory. Geoffrey W. Burr, Xin An, Fai H. Mokt, and Demetri Psaltis. Department of Electrical Engineering

Large scale rapid access holographic memory. Geoffrey W. Burr, Xin An, Fai H. Mokt, and Demetri Psaltis. Department of Electrical Engineering Large scale rapid access holographic memory Geoffrey W. Burr, Xin An, Fai H. Mokt, and Demetri Psaltis Department of Electrical Engineering California Institute of Technology, MS 116 81, Pasadena, CA 91125

More information

Design of a digital holographic interferometer for the. ZaP Flow Z-Pinch

Design of a digital holographic interferometer for the. ZaP Flow Z-Pinch Design of a digital holographic interferometer for the M. P. Ross, U. Shumlak, R. P. Golingo, B. A. Nelson, S. D. Knecht, M. C. Hughes, R. J. Oberto University of Washington, Seattle, USA Abstract The

More information

Photonic Signals. and Systems. An Introduction. NabeelA.Riza/Ph.D. Department of Electrical and Electronic Engineering University College Cork

Photonic Signals. and Systems. An Introduction. NabeelA.Riza/Ph.D. Department of Electrical and Electronic Engineering University College Cork Photonic Signals and Systems An Introduction NabeelA.Riza/Ph.D. Department of Electrical and Electronic Engineering University College Cork Cork, Ireland New York Chicago San Francisco Lisbon London Madrid

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

EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name:

EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name: EE119 Introduction to Optical Engineering Fall 2009 Final Exam Name: SID: CLOSED BOOK. THREE 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

Parallel Mode Confocal System for Wafer Bump Inspection

Parallel Mode Confocal System for Wafer Bump Inspection Parallel Mode Confocal System for Wafer Bump Inspection ECEN5616 Class Project 1 Gao Wenliang wen-liang_gao@agilent.com 1. Introduction In this paper, A parallel-mode High-speed Line-scanning confocal

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

NIR SPECTROSCOPY Instruments

NIR SPECTROSCOPY Instruments What is needed to construct a NIR instrument? NIR SPECTROSCOPY Instruments Umeå 2006-04-10 Bo Karlberg light source dispersive unit (monochromator) detector (Fibres) (bsorbance/reflectance-standard) The

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

Supplementary Information

Supplementary Information Supplementary Information Metasurface eyepiece for augmented reality Gun-Yeal Lee 1,, Jong-Young Hong 1,, SoonHyoung Hwang 2, Seokil Moon 1, Hyeokjung Kang 2, Sohee Jeon 2, Hwi Kim 3, Jun-Ho Jeong 2, and

More information

The Lightwave Model 142 CW Visible Ring Laser, Beam Splitter, Model ATM- 80A1 Acousto-Optic Modulator, and Fiber Optic Cable Coupler Optics Project

The Lightwave Model 142 CW Visible Ring Laser, Beam Splitter, Model ATM- 80A1 Acousto-Optic Modulator, and Fiber Optic Cable Coupler Optics Project The Lightwave Model 142 CW Visible Ring Laser, Beam Splitter, Model ATM- 80A1 Acousto-Optic Modulator, and Fiber Optic Cable Coupler Optics Project Stephen W. Jordan Seth Merritt Optics Project PH 464

More information

Opto-VLSI-based reconfigurable photonic RF filter

Opto-VLSI-based reconfigurable photonic RF filter Research Online ECU Publications 29 Opto-VLSI-based reconfigurable photonic RF filter Feng Xiao Mingya Shen Budi Juswardy Kamal Alameh This article was originally published as: Xiao, F., Shen, M., Juswardy,

More information

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

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember Günter Toesko - Laserseminar BLZ im Dezember 2009 1 Aberrations An optical aberration is a distortion in the image formed by an optical system compared to the original. It can arise for a number of reasons

More information

In-line digital holographic interferometry

In-line digital holographic interferometry In-line digital holographic interferometry Giancarlo Pedrini, Philipp Fröning, Henrik Fessler, and Hans J. Tiziani An optical system based on in-line digital holography for the evaluation of deformations

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

Ultralight Weight Optical Systems using Nano-Layered Synthesized Materials

Ultralight Weight Optical Systems using Nano-Layered Synthesized Materials Ultralight Weight Optical Systems using Nano-Layered Synthesized Materials Natalie Clark, PhD NASA Langley Research Center and James Breckinridge University of Arizona, College of Optical Sciences Overview

More information

Fiber Optic Communications

Fiber Optic Communications Fiber Optic Communications ( Chapter 2: Optics Review ) presented by Prof. Kwang-Chun Ho 1 Section 2.4: Numerical Aperture Consider an optical receiver: where the diameter of photodetector surface area

More information

Copyright 2009 SPIE and IS&T. This paper was (will be) published in Proceedings Electronic Imaging 2009 and is made available as an electronic

Copyright 2009 SPIE and IS&T. This paper was (will be) published in Proceedings Electronic Imaging 2009 and is made available as an electronic Copyright 2009 SPIE and IS&T. This paper was (will be) published in Proceedings Electronic Imaging 2009 and is made available as an electronic reprint (preprint) with permission of SPIE and IS&T. One print

More information

Gerhard K. Ackermann and Jurgen Eichler. Holography. A Practical Approach BICENTENNIAL. WILEY-VCH Verlag GmbH & Co. KGaA

Gerhard K. Ackermann and Jurgen Eichler. Holography. A Practical Approach BICENTENNIAL. WILEY-VCH Verlag GmbH & Co. KGaA Gerhard K. Ackermann and Jurgen Eichler Holography A Practical Approach BICENTENNIAL BICENTENNIAL WILEY-VCH Verlag GmbH & Co. KGaA Contents Preface XVII Part 1 Fundamentals of Holography 1 1 Introduction

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

Chapter 4: Fourier Optics

Chapter 4: Fourier Optics Chapter 4: Fourier Optics P4-1. Calculate the Fourier transform of the function rect(2x)rect(/3) The rectangular function rect(x) is given b 1 x 1/2 rect( x) when 0 x 1/2 P4-2. Assume that ( gx (, )) G

More information

PHY 431 Homework Set #5 Due Nov. 20 at the start of class

PHY 431 Homework Set #5 Due Nov. 20 at the start of class PHY 431 Homework Set #5 Due Nov. 0 at the start of class 1) Newton s rings (10%) The radius of curvature of the convex surface of a plano-convex lens is 30 cm. The lens is placed with its convex side down

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

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

25 cm. 60 cm. 50 cm. 40 cm. Geometrical Optics 7. The image formed by a plane mirror is: (a) Real. (b) Virtual. (c) Erect and of equal size. (d) Laterally inverted. (e) B, c, and d. (f) A, b and c. 8. A real image is that: (a) Which

More information

Diffractive optical elements based on Fourier optical techniques: a new class of optics for extreme ultraviolet and soft x-ray wavelengths

Diffractive optical elements based on Fourier optical techniques: a new class of optics for extreme ultraviolet and soft x-ray wavelengths Diffractive optical elements based on Fourier optical techniques: a new class of optics for extreme ultraviolet and soft x-ray wavelengths Chang Chang, Patrick Naulleau, Erik Anderson, Kristine Rosfjord,

More information

Department of Mechanical and Aerospace Engineering, Princeton University Department of Astrophysical Sciences, Princeton University ABSTRACT

Department of Mechanical and Aerospace Engineering, Princeton University Department of Astrophysical Sciences, Princeton University ABSTRACT Phase and Amplitude Control Ability using Spatial Light Modulators and Zero Path Length Difference Michelson Interferometer Michael G. Littman, Michael Carr, Jim Leighton, Ezekiel Burke, David Spergel

More information

Fast, Two-Dimensional Optical Beamscanning by Wavelength Switching T. K. Chan, E. Myslivets, J. E. Ford

Fast, Two-Dimensional Optical Beamscanning by Wavelength Switching T. K. Chan, E. Myslivets, J. E. Ford Photonics Systems Integration Lab University of California San Diego Jacobs School of Engineering Fast, Two-Dimensional Optical Beamscanning by Wavelength Switching T. K. Chan, E. Myslivets, J. E. Ford

More information

Optical Information Processing. Adolf W. Lohmann. Edited by Stefan Sinzinger. Ch>

Optical Information Processing. Adolf W. Lohmann. Edited by Stefan Sinzinger. Ch> Optical Information Processing Adolf W. Lohmann Edited by Stefan Sinzinger Ch> Universitätsverlag Ilmenau 2006 Contents Preface to the 2006 edition 13 Preface to the third edition 15 Preface volume 1 17

More information

Research Trends in Spatial Imaging 3D Video

Research Trends in Spatial Imaging 3D Video Research Trends in Spatial Imaging 3D Video Spatial image reproduction 3D video (hereinafter called spatial image reproduction ) is able to display natural 3D images without special glasses. Its principles

More information

A wavefront generator for complex pupil function synthesis and point spread function engineering

A wavefront generator for complex pupil function synthesis and point spread function engineering Journal of Microscopy, Vol. 197, Pt 3, March 2000, pp. 219±223. Received 27 September 1999; accepted 30 November 1999 SHORT COMMUNICATION A wavefront generator for complex pupil function synthesis and

More information

Holography as a tool for advanced learning of optics and photonics

Holography as a tool for advanced learning of optics and photonics Holography as a tool for advanced learning of optics and photonics Victor V. Dyomin, Igor G. Polovtsev, Alexey S. Olshukov Tomsk State University 36 Lenin Avenue, Tomsk, 634050, Russia Tel/fax: 7 3822

More information

Name Class Date. Use the terms from the following list to complete the sentences below. Each term may be used only once. Some terms may not be used.

Name Class Date. Use the terms from the following list to complete the sentences below. Each term may be used only once. Some terms may not be used. Assessment Chapter Test B Light and Our World USING KEY TERMS Use the terms from the following list to complete the sentences below. Each term may be used only once. Some terms may not be used. concave

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Optically reconfigurable metasurfaces and photonic devices based on phase change materials S1: Schematic diagram of the experimental setup. A Ti-Sapphire femtosecond laser (Coherent Chameleon Vision S)

More information

Chapter Ray and Wave Optics

Chapter Ray and Wave Optics 109 Chapter Ray and Wave Optics 1. An astronomical telescope has a large aperture to [2002] reduce spherical aberration have high resolution increase span of observation have low dispersion. 2. If two

More information

GENERATION OF SPATIAL LIGHT DISTRIBUTIONS

GENERATION OF SPATIAL LIGHT DISTRIBUTIONS GENERATION OF SPATIAL LIGHT DISTRIBUTIONS PhD theses LÁSZLÓ DOMJÁN TUTOR: DR. LÁSZLÓ KOCSÁNYI DOCENT Department of Atomic Physics Faculty of Natural Sciences TU Budapest 2004 1. Introduction A spatial

More information

Optical Signal Processing

Optical Signal Processing Optical Signal Processing ANTHONY VANDERLUGT North Carolina State University Raleigh, North Carolina A Wiley-Interscience Publication John Wiley & Sons, Inc. New York / Chichester / Brisbane / Toronto

More information

Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy

Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy Qiyuan Song (M2) and Aoi Nakamura (B4) Abstracts: We theoretically and experimentally

More information

Increasing pixel count of holograms for three-dimensional holographic display by optical scan-tiling

Increasing pixel count of holograms for three-dimensional holographic display by optical scan-tiling Increasing pixel count of holograms for three-dimensional holographic display by optical scan-tiling Zhi Ming Abel Lum Xinan Liang Yuechao Pan Ruitao Zheng Xuewu Xu Optical Engineering 52(1), 015802 (January

More information

A simple and effective first optical image processing experiment

A simple and effective first optical image processing experiment A simple and effective first optical image processing experiment Dale W. Olson Physics Department, University of Northern Iowa, Cedar Falls, IA 50614-0150 Abstract: Optical image processing experiments

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

Spatial Light Modulator (SLM) Workshop, BFY 2012 Conference Douglas Martin and Shannon O Leary Lawrence University and Lewis & Clark College

Spatial Light Modulator (SLM) Workshop, BFY 2012 Conference Douglas Martin and Shannon O Leary Lawrence University and Lewis & Clark College Spatial Light Modulator (SLM) Workshop, BFY 2012 Conference Douglas Martin and Shannon O Leary Lawrence University and Lewis & Clark College Briefly, a spatial light modulator (SLM) is a liquid crystal

More information

Pulse Shaping Application Note

Pulse Shaping Application Note Application Note 8010 Pulse Shaping Application Note Revision 1.0 Boulder Nonlinear Systems, Inc. 450 Courtney Way Lafayette, CO 80026-8878 USA Shaping ultrafast optical pulses with liquid crystal spatial

More information

Sinusoidal wavelength-scanning common-path interferometer with a beam-scanning system for measurement of film thickness variations

Sinusoidal wavelength-scanning common-path interferometer with a beam-scanning system for measurement of film thickness variations Sinusoidal wavelength-scanning common-path interferometer with a beam-scanning system for measurement of film thickness variations Osami Sasaki, Takafumi Morimatsu, Samuel Choi, and Takamasa Suzuki Faculty

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

on the absence of phase-recording or twin-image

on the absence of phase-recording or twin-image BRIT, J. APPL. PHYS., 1966, VOL. 17 on the absence of phase-recording or twin-image separation problems in abor (in-line) o ~ o ~ ~ a G. W. STROKE, D. BRUMM, A. FUNKHOUSER, A. LABEYRIE and R. C. RESTRICK

More information

Inverted-COR: Inverted-Occultation Coronagraph for Solar Orbiter

Inverted-COR: Inverted-Occultation Coronagraph for Solar Orbiter Inverted-COR: Inverted-Occultation Coronagraph for Solar Orbiter OATo Technical Report Nr. 119 Date 19-05-2009 by: Silvano Fineschi Release Date Sheet: 1 of 1 REV/ VER LEVEL DOCUMENT CHANGE RECORD DESCRIPTION

More information

Adaptive multi/demultiplexers for optical signals with arbitrary wavelength spacing.

Adaptive multi/demultiplexers for optical signals with arbitrary wavelength spacing. Edith Cowan University Research Online ECU Publications Pre. 2011 2010 Adaptive multi/demultiplexers for optical signals with arbitrary wavelength spacing. Feng Xiao Edith Cowan University Kamal Alameh

More information

microscopy A great online resource Molecular Expressions, a Microscope Primer Partha Roy

microscopy A great online resource Molecular Expressions, a Microscope Primer Partha Roy Fundamentals of optical microscopy A great online resource Molecular Expressions, a Microscope Primer http://micro.magnet.fsu.edu/primer/index.html Partha Roy 1 Why microscopy Topics Functions of a microscope

More information

Wavelength Stabilization of HPDL Array Fast-Axis Collimation Optic with integrated VHG

Wavelength Stabilization of HPDL Array Fast-Axis Collimation Optic with integrated VHG Wavelength Stabilization of HPDL Array Fast-Axis Collimation Optic with integrated VHG C. Schnitzler a, S. Hambuecker a, O. Ruebenach a, V. Sinhoff a, G. Steckman b, L. West b, C. Wessling c, D. Hoffmann

More information

BEAM HALO OBSERVATION BY CORONAGRAPH

BEAM HALO OBSERVATION BY CORONAGRAPH BEAM HALO OBSERVATION BY CORONAGRAPH T. Mitsuhashi, KEK, TSUKUBA, Japan Abstract We have developed a coronagraph for the observation of the beam halo surrounding a beam. An opaque disk is set in the beam

More information

Metrology and Sensing

Metrology and Sensing Metrology and Sensing Lecture 10: Holography 2017-12-21 Herbert Gross Winter term 2017 www.iap.uni-jena.de 2 Preliminary Schedule No Date Subject Detailed Content 1 19.10. Introduction Introduction, optical

More information

Development of a new multi-wavelength confocal surface profilometer for in-situ automatic optical inspection (AOI)

Development of a new multi-wavelength confocal surface profilometer for in-situ automatic optical inspection (AOI) Development of a new multi-wavelength confocal surface profilometer for in-situ automatic optical inspection (AOI) Liang-Chia Chen 1#, Chao-Nan Chen 1 and Yi-Wei Chang 1 1. Institute of Automation Technology,

More information

Rotation/ scale invariant hybrid digital/optical correlator system for automatic target recognition

Rotation/ scale invariant hybrid digital/optical correlator system for automatic target recognition Rotation/ scale invariant hybrid digital/optical correlator system for automatic target recognition V. K. Beri, Amit Aran, Shilpi Goyal, and A. K. Gupta * Photonics Division Instruments Research and Development

More information

Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature:

Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature: Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: PID: Signature: CLOSED BOOK. TWO 8 1/2 X 11 SHEET OF NOTES (double sided is allowed), AND SCIENTIFIC POCKET CALCULATOR

More information

Week IV: FIRST EXPERIMENTS WITH THE ADVANCED OPTICS SET

Week IV: FIRST EXPERIMENTS WITH THE ADVANCED OPTICS SET Week IV: FIRST EXPERIMENTS WITH THE ADVANCED OPTICS SET The Advanced Optics set consists of (A) Incandescent Lamp (B) Laser (C) Optical Bench (with magnetic surface and metric scale) (D) Component Carriers

More information

Holographic Optical Tweezers and High-speed imaging. Miles Padgett, Department of Physics and Astronomy

Holographic Optical Tweezers and High-speed imaging. Miles Padgett, Department of Physics and Astronomy Holographic Optical Tweezers and High-speed imaging Miles Padgett, Department of Physics and Astronomy High-speed Imaging in Optical Tweezers Holographic Optical Tweezers Tweezers human interface, the

More information

A liquid crystal spatial light phase modulator and its applications

A liquid crystal spatial light phase modulator and its applications Invited Paper A liquid crystal spatial light phase modulator and its applications Tsutomu Hara Central Research Laboratory; Hamamatsu Photonics K.K. 5000 Hirakuchi, Hamakita-City, Shizuoka-Prefecture,

More information

2.C A New Shearing Interferometer for Real-Time Characterization of Cryogenic Laser-Fusion Targets

2.C A New Shearing Interferometer for Real-Time Characterization of Cryogenic Laser-Fusion Targets LLE REVIEW, Volume 40 9. V. Varadarajan, K. Kim, and T. P. Bernat, J. Vac. Sci. Technol. A 5, 2750 (1987). 10. L. S. Mok and K. Kim, J. Fluid Mech. 176, 521 (1987). 11. K. Kim, L. Mok, M. J. Erlenborn,

More information

VC 11/12 T2 Image Formation

VC 11/12 T2 Image Formation VC 11/12 T2 Image Formation Mestrado em Ciência de Computadores Mestrado Integrado em Engenharia de Redes e Sistemas Informáticos Miguel Tavares Coimbra Outline Computer Vision? The Human Visual System

More information

Be aware that there is no universal notation for the various quantities.

Be aware that there is no universal notation for the various quantities. Fourier Optics v2.4 Ray tracing is limited in its ability to describe optics because it ignores the wave properties of light. Diffraction is needed to explain image spatial resolution and contrast and

More information

Module 19 : WDM Components

Module 19 : WDM Components Module 19 : WDM Components Lecture : WDM Components - I Part - I Objectives In this lecture you will learn the following WDM Components Optical Couplers Optical Amplifiers Multiplexers (MUX) Insertion

More information

A High-Concentration Programmable Solar Simulator for Testing Multi-Junction Concentrator Photovoltaics

A High-Concentration Programmable Solar Simulator for Testing Multi-Junction Concentrator Photovoltaics A High-Concentration Programmable Solar Simulator for Testing ulti-junction Concentrator Photovoltaics Tasshi Dennis 1, Brent Fisher 2, att eitl 2, and John Wilson 2 1 National Institute of Standards and

More information

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

Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California Modern Optical Engineering The Design of Optical Systems Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California Fourth Edition Me Graw Hill New York Chicago San Francisco

More information

Deep Horizontal Atmospheric Turbulence Modeling and Simulation with a Liquid Crystal Spatial Light Modulator. *Corresponding author:

Deep Horizontal Atmospheric Turbulence Modeling and Simulation with a Liquid Crystal Spatial Light Modulator. *Corresponding author: Deep Horizontal Atmospheric Turbulence Modeling and Simulation with a Liquid Crystal Spatial Light Modulator Peter Jacquemin a*, Bautista Fernandez a, Christopher C. Wilcox b, Ty Martinez b, Brij Agrawal

More information

Coherent, focus-corrected imaging of optical fiber facets using a single-pixel detector

Coherent, focus-corrected imaging of optical fiber facets using a single-pixel detector Coherent, focus-corrected imaging of optical fiber facets using a single-pixel detector George S. D. Gordon, 1, Feng Feng, 1 Qiongyue Kang, 2 Yongmin Jung, 2 and Jayanta Sahu, 2 and Timothy Wilkinson 1

More information

ECEN. Spectroscopy. Lab 8. copy. constituents HOMEWORK PR. Figure. 1. Layout of. of the

ECEN. Spectroscopy. Lab 8. copy. constituents HOMEWORK PR. Figure. 1. Layout of. of the ECEN 4606 Lab 8 Spectroscopy SUMMARY: ROBLEM 1: Pedrotti 3 12-10. In this lab, you will design, build and test an optical spectrum analyzer and use it for both absorption and emission spectroscopy. The

More information

J. C. Wyant Fall, 2012 Optics Optical Testing and Testing Instrumentation

J. C. Wyant Fall, 2012 Optics Optical Testing and Testing Instrumentation J. C. Wyant Fall, 2012 Optics 513 - Optical Testing and Testing Instrumentation Introduction 1. Measurement of Paraxial Properties of Optical Systems 1.1 Thin Lenses 1.1.1 Measurements Based on Image Equation

More information

R.B.V.R.R. WOMEN S COLLEGE (AUTONOMOUS) Narayanaguda, Hyderabad.

R.B.V.R.R. WOMEN S COLLEGE (AUTONOMOUS) Narayanaguda, Hyderabad. R.B.V.R.R. WOMEN S COLLEGE (AUTONOMOUS) Narayanaguda, Hyderabad. DEPARTMENT OF PHYSICS QUESTION BANK FOR SEMESTER III PAPER III OPTICS UNIT I: 1. MATRIX METHODS IN PARAXIAL OPTICS 2. ABERATIONS UNIT II

More information

Laser Telemetric System (Metrology)

Laser Telemetric System (Metrology) Laser Telemetric System (Metrology) Laser telemetric system is a non-contact gauge that measures with a collimated laser beam (Refer Fig. 10.26). It measure at the rate of 150 scans per second. It basically

More information

MEASUREMENT OF HOLOGRAPHIC TRAP POSITIONING

MEASUREMENT OF HOLOGRAPHIC TRAP POSITIONING MSc in Photonics Universitat Politècnica de Catalunya (UPC) Universitat Autònoma de Barcelona (UAB) Universitat de Barcelona (UB) Institut de Ciències Fotòniques (ICFO) PHOTONICSBCN http://www.photonicsbcn.eu

More information

LOS 1 LASER OPTICS SET

LOS 1 LASER OPTICS SET LOS 1 LASER OPTICS SET Contents 1 Introduction 3 2 Light interference 5 2.1 Light interference on a thin glass plate 6 2.2 Michelson s interferometer 7 3 Light diffraction 13 3.1 Light diffraction on a

More information

Sensitive measurement of partial coherence using a pinhole array

Sensitive measurement of partial coherence using a pinhole array 1.3 Sensitive measurement of partial coherence using a pinhole array Paul Petruck 1, Rainer Riesenberg 1, Richard Kowarschik 2 1 Institute of Photonic Technology, Albert-Einstein-Strasse 9, 07747 Jena,

More information

Sintec Optronics Technology Pte Ltd 10 Bukit Batok Crescent #07-02 The Spire Singapore Tel: Fax:

Sintec Optronics Technology Pte Ltd 10 Bukit Batok Crescent #07-02 The Spire Singapore Tel: Fax: Sintec Optronics Technology Pte Ltd 10 Bukit Batok Crescent #07-02 The Spire Singapore 658079 Tel: +65 63167112 Fax: +65 63167113 High-power Nd:YAG Self-floating Laser Cutting Head We supply the laser

More information

Chapter 23 Study Questions Name: Class:

Chapter 23 Study Questions Name: Class: Chapter 23 Study Questions Name: Class: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. 1. When you look at yourself in a plane mirror, you

More information

APPLICATION OF A POINT-DIFFRACTION INTERFEROMETER TO UNSTEADY SHOCK WAVE PHENOMENA

APPLICATION OF A POINT-DIFFRACTION INTERFEROMETER TO UNSTEADY SHOCK WAVE PHENOMENA 15 th International Symposium on Flow Visualization June 25-28, 2012, Minsk, Belarus APPLICATION OF A POINT-DIFFRACTION INTERFEROMETER Daiju Numata 1,c, Kiyonobu Ohtani 2 1 Tohoku University, 6-6-01 Aramaki-Aza-Aoba,

More information

Wuxi OptonTech Ltd. Structured light DOEs without requiring collimation: For surface-emitting lasers (e.g. VCSELs)

Wuxi OptonTech Ltd. Structured light DOEs without requiring collimation: For surface-emitting lasers (e.g. VCSELs) . specializes in diffractive optical elements (DOEs) and computer generated holograms (CGHs)for beam shaping, beam splitting and beam homogenizing (diffusing). We design and provide standard and custom

More information

Speckle free laser projection

Speckle free laser projection Speckle free laser projection With Optotune s Laser Speckle Reducer October 2013 Dr. Selina Casutt, Application Engineer Bernstrasse 388 CH-8953 Dietikon Switzerland Phone +41 58 856 3011 www.optotune.com

More information

Dynamic Opto-VLSI lens and lens-let generation with programmable focal length

Dynamic Opto-VLSI lens and lens-let generation with programmable focal length Edith Cowan University Research Online ECU Publications Pre. 2011 2005 Dynamic Opto-VLSI lens and lens-let generation with programmable focal length Zhenglin Wang Edith Cowan University Kamal Alameh Edith

More information