Holography October, 2006
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Comparison Between Digital Fresnel Holography and Digital Image-Plane Holography: the Role of the Imaging Aperture M
Comparison between Digital Fresnel Holography and Digital Image-Plane Holography: The Role of the Imaging Aperture M. Karray, Pierre Slangen, Pascal Picart To cite this version: M. Karray, Pierre Slangen, Pascal Picart. Comparison between Digital Fresnel Holography and Digital Image-Plane Holography: The Role of the Imaging Aperture. Experimental Mechanics, Society for Experimental Mechanics, 2012, 52 (9), pp.1275-1286. 10.1007/s11340-012-9604-6. hal-02012133 HAL Id: hal-02012133 https://hal.archives-ouvertes.fr/hal-02012133 Submitted on 26 Feb 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Comparison between Digital Fresnel Holography and Digital Image-Plane Holography: The Role of the Imaging Aperture M. Karray & P. Slangen & P. Picart Abstract Optical techniques are now broadly used in the experimental analysis. Particularly, a theoretical analysis field of experimental mechanics. The main advantages are of the influence of the aperture and lens in the case of they are non intrusive and no contact. Moreover optical image-plane holography is proposed. Optimal filtering techniques lead to full spatial resolution displacement maps and image recovering conditions are thus established. enabling the computing of mechanical value also in high Experimental results show the appropriateness of the spatial resolution. -
Digital Holography Using a Laser Pointer and Consumer Digital Camera Report Date: June 22Nd, 2004
Digital Holography using a Laser Pointer and Consumer Digital Camera Report date: June 22nd, 2004 by David Garber, M.E. undergraduate, Johns Hopkins University, [email protected] Available online at http://pegasus.me.jhu.edu/~lefd/shc/LPholo/lphindex.htm Acknowledgements Faculty sponsor: Prof. Joseph Katz, [email protected] Project idea and direction: Dr. Edwin Malkiel, [email protected] Digital holography reconstruction: Jian Sheng, [email protected] Abstract The point of this project was to examine the feasibility of low-cost holography. Can viable holograms be recorded using an ordinary diode laser pointer and a consumer digital camera? How much does it cost? What are the major difficulties? I set up an in-line holographic system and recorded both still images and movies using a $600 Fujifilm Finepix S602Z digital camera and a $10 laser pointer by Lazerpro. Reconstruction of the stills shows clearly that successful holograms can be created with a low-cost optical setup. The movies did not reconstruct, due to compression and very low image resolution. Garber 2 Theoretical Background What is a hologram? The Merriam-Webster dictionary defines a hologram as, “a three-dimensional image reproduced from a pattern of interference produced by a split coherent beam of radiation (as a laser).” Holograms can produce a three-dimensional image, but it is more helpful for our purposes to think of a hologram as a photograph that can be refocused at any depth. So while a photograph taken of two people standing far apart would have one in focus and one blurry, a hologram taken of the same scene could be reconstructed to bring either person into focus. -
The Slide Projector As a Computer-Operated Visual Display*
SESSION III CONTRIBUTED PAPERS: PROCESS CONTROL (INTRODUCTORY) Robert S. Mcl.ean. Ontario Institute for Studies in Education, Presider The slide projector as a computer-operated visual display* PAUL B. BUCKLEY and CLIFFORD B. GILLMAN have had experience with slides and can generate University of Wisconsin, Madison, Wisconsin 53706 appropriate stimuli easily. Furthermore, changing or .supplementing the stimulus set requires no new Advantages and method are presented for using the programming and no additional memory storage. slide projector in a computer-operated visual display Interfacing an inexpensive tachistoscope to the system. computer may also meet the E's requirements for a visual display. However, the projector is more flexible in The presentation of visual stimuli is a common that one can display many stimuli without E procedure in psychological research (Aaronson & intervention. so that intertrial interval is precisely Brauth, 1972). For example, visual stimuli have been controlled. Furthermore, two projectors with employed in our laboratory for experiments in superimposed images, paired in the proper timing perception, learning, memory, choice reaction time, and se q uence, c an perfectly mimic a two-channel very short-term memory. Obviously, this is not an tachistoscope. The shutter on one projector is exhaustive list of potential uses. In the programmed to open as the shutter on the other computer-controlled laboratory, the cathode ray projector closes. Thirdly, whereas a tachistoscope may terminal (CRT) or oscilloscope (CRO) may be used to be used to test one S at a time, a pair of projectors meet this need (Sperling, 1971 ; Van Gelder, 1972; simulating a tachistoscope may present material to Wojnarowski, Bachman, & Pollack, 1971). -
Scanning Camera for Continuous-Wave Acoustic Holography
Scanning Camera for Continuous-Wave Acoustic Holography Hillary W. Gao, Kimberly I. Mishra, Annemarie Winters, Sidney Wolin, and David G. Griera) Department of Physics and Center for Soft Matter Research, New York University, New York, NY 10003, USA (Dated: 7 August 2018) 1 We present a system for measuring the amplitude and phase profiles of the pressure 2 field of a harmonic acoustic wave with the goal of reconstructing the volumetric sound 3 field. Unlike optical holograms that cannot be reconstructed exactly because of the 4 inverse problem, acoustic holograms are completely specified in the recording plane. 5 We demonstrate volumetric reconstructions of simple arrangements of objects using 6 the Rayleigh-Sommerfeld diffraction integral, and introduce a technique to analyze 7 the dynamic properties of insonated objects. a)[email protected] 1 Scanning Holographic Camera 8 Most technologies for acoustic imaging use the temporal and spectral characteristics of 1 9 acoustic pulses to map interfaces between distinct phases. This is the basis for sonar , and 2 10 medical and industrial ultrasonography . Imaging continuous-wave sound fields is useful for 3 11 industrial and environmental noise analysis, particularly for source localization . Substan- 12 tially less attention has been paid to visualizing the amplitude and phase profiles of sound 13 fields for their own sakes, with most effort being focused on visualizing the near-field acous- 14 tic radiation emitted by localized sources, a technique known as near-field acoustic holog- 4{6 15 raphy (NAH) . The advent of acoustic manipulation in holographically structured sound 7{11 16 fields creates a need for effective sound-field visualization. -
Ground-Based Photographic Monitoring
United States Department of Agriculture Ground-Based Forest Service Pacific Northwest Research Station Photographic General Technical Report PNW-GTR-503 Monitoring May 2001 Frederick C. Hall Author Frederick C. Hall is senior plant ecologist, U.S. Department of Agriculture, Forest Service, Pacific Northwest Region, Natural Resources, P.O. Box 3623, Portland, Oregon 97208-3623. Paper prepared in cooperation with the Pacific Northwest Region. Abstract Hall, Frederick C. 2001 Ground-based photographic monitoring. Gen. Tech. Rep. PNW-GTR-503. Portland, OR: U.S. Department of Agriculture, Forest Service, Pacific Northwest Research Station. 340 p. Land management professionals (foresters, wildlife biologists, range managers, and land managers such as ranchers and forest land owners) often have need to evaluate their management activities. Photographic monitoring is a fast, simple, and effective way to determine if changes made to an area have been successful. Ground-based photo monitoring means using photographs taken at a specific site to monitor conditions or change. It may be divided into two systems: (1) comparison photos, whereby a photograph is used to compare a known condition with field conditions to estimate some parameter of the field condition; and (2) repeat photo- graphs, whereby several pictures are taken of the same tract of ground over time to detect change. Comparison systems deal with fuel loading, herbage utilization, and public reaction to scenery. Repeat photography is discussed in relation to land- scape, remote, and site-specific systems. Critical attributes of repeat photography are (1) maps to find the sampling location and of the photo monitoring layout; (2) documentation of the monitoring system to include purpose, camera and film, w e a t h e r, season, sampling technique, and equipment; and (3) precise replication of photographs. -
Digital Refocusing with Incoherent Holography
Digital Refocusing with Incoherent Holography Oliver Cossairt Nathan Matsuda Northwestern University Northwestern University Evanston, IL Evanston, IL [email protected] [email protected] Mohit Gupta Columbia University New York, NY [email protected] Abstract ‘adding’ and ‘subtracting’ blur to the point spread functions (PSF) of different scene points, depending on their depth. In Light field cameras allow us to digitally refocus a pho- a conventional 2D image, while it is possible to add blur to tograph after the time of capture. However, recording a a scene point’s PSF, it is not possible to subtract or remove light field requires either a significant loss in spatial res- blur without introducing artifacts in the image. This is be- olution [10, 20, 9] or a large number of images to be cap- cause 2D imaging is an inherently lossy process; the angular tured [11]. In this paper, we propose incoherent hologra- information in the 4D light field is lost in a 2D image. Thus, phy for digital refocusing without loss of spatial resolution typically, if digital refocusing is desired, 4D light fields are from only 3 captured images. The main idea is to cap- captured. Unfortunately, light field cameras sacrifice spa- ture 2D coherent holograms of the scene instead of the 4D tial resolution in order to capture the angular information. light fields. The key properties of coherent light propagation The loss in resolution can be significant, up to 1-2 orders are that the coherent spread function (hologram of a single of magnitude. While there have been attempts to improve point source) encodes scene depths and has a broadband resolution by using compressive sensing techniques [14], spatial frequency response. -
Lenses and Optical Instruments
INSTITUTE FOR NANOSTRUCTURE - AND SOLID STATE PHYSICS LABORATORY EXPERIMENTS IN PHYSICS FOR ENGINEERING STUDENTS HAMBURG UNIVERSITY , JUNGIUSSTRAßE 11 Lenses and optical instruments 1. Basic Theory The aim of this experiment is to determine the focal lengths of several different lenses. Afterwards we will use these lenses to build some simple optical instruments. First, we consider image formation by thin lenses. The relationship between the focal length f of a lens, the object distance g, and the image distance b determines the ratio of the image height B to the object height G. In Fig. 1 the two right-angled triangles on the left and right sides of the lens are similar. Figure 1: Construction to find the image position (1) for a thin lens using three principal rays: i.e. the = = focal-, parallel-, and central rays. − We can rearrange this equation to get the lens equation for thin lenses: 1 1 1 or . (2) = + = + The imaging behavior of the lens depends on whether the object is located outside the first focal point, at the focal point, or inside the focal point, as shown in this table: Object Image Position g Type Position Orientation Relative size ∞ real b = f -/- point ∞ > g > 2 f real f < b < 2f inverted demagnified g = 2 f real b = 2f inverted equal size f < g < 2 f real ∞ > b > 2f inverted magnified g = f ∞ g < f virtual |b| > g upright magnified 1 Lenses and optical instruments 2. Experimental Procedure 2.1 Determining the focal length of a lens Measuring image and object distances. In this experiment the focal lengths of two different converging lenses are to be determined by measuring the image distance b and object distance g (see Fig.1) for each lens. -
American Scientist the Magazine of Sigma Xi, the Scientific Research Society
A reprint from American Scientist the magazine of Sigma Xi, The Scientific Research Society This reprint is provided for personal and noncommercial use. For any other use, please send a request to Permissions, American Scientist, P.O. Box 13975, Research Triangle Park, NC, 27709, U.S.A., or by electronic mail to [email protected]. ©Sigma Xi, The Scientific Research Society and other rightsholders Engineering Next Slide, Please Henry Petroski n the course of preparing lectures years—against strong opposition from Ibased on the material in my books As the Kodak some in the artistic community—that and columns, I developed during the simple projection devices were used by closing decades of the 20th century a the masters to trace in near exactness good-sized library of 35-millimeter Carousel begins its intricate images, including portraits, that slides. These show structures large and the free hand could not do with fidelity. small, ranging from bridges and build- slide into history, ings to pencils and paperclips. As re- The Magic Lantern cently as about five years ago, when I it joins a series of The most immediate antecedent of the indicated to a host that I would need modern slide projector was the magic the use of a projector during a talk, just previous devices used lantern, a device that might be thought about everyone understood that to mean of as a camera obscura in reverse. Instead a Kodak 35-mm slide projector (or its to add images to talks of squeezing a life-size image through a equivalent), and just about every venue pinhole to produce an inverted minia- had one readily available. -
A Curriculum Guide
FOCUS ON PHOTOGRAPHY: A CURRICULUM GUIDE This page is an excerpt from Focus on Photography: A Curriculum Guide Written by Cynthia Way for the International Center of Photography © 2006 International Center of Photography All rights reserved. Published by the International Center of Photography, New York. Printed in the United States of America. Please credit the International Center of Photography on all reproductions. This project has been made possible with generous support from Andrew and Marina Lewin, the GE Fund, and public funds from the New York City Department of Cultural Affairs Cultural Challenge Program. FOCUS ON PHOTOGRAPHY: A CURRICULUM GUIDE PART IV Resources FOCUS ON PHOTOGRAPHY: A CURRICULUM GUIDE This section is an excerpt from Focus on Photography: A Curriculum Guide Written by Cynthia Way for the International Center of Photography © 2006 International Center of Photography All rights reserved. Published by the International Center of Photography, New York. Printed in the United States of America. Please credit the International Center of Photography on all reproductions. This project has been made possible with generous support from Andrew and Marina Lewin, the GE Fund, and public funds from the New York City Department of Cultural Affairs Cultural Challenge Program. FOCUS ON PHOTOGRAPHY: A CURRICULUM GUIDE Focus Lesson Plans Fand Actvities INDEX TO FOCUS LINKS Focus Links Lesson Plans Focus Link 1 LESSON 1: Introductory Polaroid Exercises Focus Link 2 LESSON 2: Camera as a Tool Focus Link 3 LESSON 3: Photographic Field -
State-Of-The-Art in Holography and Auto-Stereoscopic Displays
State-of-the-art in holography and auto-stereoscopic displays Daniel Jönsson <Ersätt med egen bild> 2019-05-13 Contents Introduction .................................................................................................................................................. 3 Auto-stereoscopic displays ........................................................................................................................... 5 Two-View Autostereoscopic Displays ....................................................................................................... 5 Multi-view Autostereoscopic Displays ...................................................................................................... 7 Light Field Displays .................................................................................................................................. 10 Market ......................................................................................................................................................... 14 Display panels ......................................................................................................................................... 14 AR ............................................................................................................................................................ 14 Application Fields ........................................................................................................................................ 15 Companies ................................................................................................................................................. -
Full-Color See-Through Three-Dimensional Display Method Based on Volume Holography
sensors Article Full-Color See-Through Three-Dimensional Display Method Based on Volume Holography Taihui Wu 1,2 , Jianshe Ma 2, Chengchen Wang 1,2, Haibei Wang 2 and Ping Su 2,* 1 Department of Precision Instrument, Tsinghua University, Beijing 100084, China; [email protected] (T.W.); [email protected] (C.W.) 2 Tsinghua Shenzhen International Graduate School, Tsinghua University, Shenzhen 518055, China; [email protected] (J.M.); [email protected] (H.W.) * Correspondence: [email protected] Abstract: We propose a full-color see-through three-dimensional (3D) display method based on volume holography. This method is based on real object interference, avoiding the device limitation of spatial light modulator (SLM). The volume holography has a slim and compact structure, which realizes 3D display through one single layer of photopolymer. We analyzed the recording mechanism of volume holographic gratings, diffraction characteristics, and influencing factors of refractive index modulation through Kogelnik’s coupled-wave theory and the monomer diffusion model of photopolymer. We built a multiplexing full-color reflective volume holographic recording optical system and conducted simultaneous exposure experiment. Under the illumination of white light, full-color 3D image can be reconstructed. Experimental results show that the average diffraction efficiency is about 53%, and the grating fringe pitch is less than 0.3 µm. The reconstructed image of volume holography has high diffraction efficiency, high resolution, strong stereo perception, and large observing angle, which provides a technical reference for augmented reality. Citation: Wu, T.; Ma, J.; Wang, C.; Keywords: holographic display; volume holography; photopolymer; augmented reality Wang, H.; Su, P. -
3D-Integrated Metasurfaces for Full-Colour Holography Yueqiang Hu 1, Xuhao Luo1, Yiqin Chen1, Qing Liu1,Xinli1,Yasiwang1,Naliu2 and Huigao Duan1
Hu et al. Light: Science & Applications (2019) 8:86 Official journal of the CIOMP 2047-7538 https://doi.org/10.1038/s41377-019-0198-y www.nature.com/lsa ARTICLE Open Access 3D-Integrated metasurfaces for full-colour holography Yueqiang Hu 1, Xuhao Luo1, Yiqin Chen1, Qing Liu1,XinLi1,YasiWang1,NaLiu2 and Huigao Duan1 Abstract Metasurfaces enable the design of optical elements by engineering the wavefront of light at the subwavelength scale. Due to their ultrathin and compact characteristics, metasurfaces possess great potential to integrate multiple functions in optoelectronic systems for optical device miniaturisation. However, current research based on multiplexing in the 2D plane has not fully utilised the capabilities of metasurfaces for multi-tasking applications. Here, we demonstrate a 3D-integrated metasurface device by stacking a hologram metasurface on a monolithic Fabry–Pérot cavity-based colour filter microarray to simultaneously achieve low-crosstalk, polarisation-independent, high-efficiency, full-colour holography, and microprint. The dual functions of the device outline a novel scheme for data recording, security encryption, colour displays, and information processing. Our 3D integration concept can be extended to achieve multi-tasking flat optical systems by including a variety of functional metasurface layers, such as polarizers, metalenses, and others. Introduction dimensional (3D) integration of discrete metasurfaces. For 1234567890():,; 1234567890():,; 1234567890():,; 1234567890():,; Metasurfaces open a new paradigm to design optical example, anisotropic structures or interleaved subarrays elements by shaping the wavefront of electromagnetic have been specifically arranged in a 2D plane to obtain – waves by tailoring the size, shape, and arrangement of multiplexed devices10,16 18. To reduce crosstalk, plas- – subwavelength structures1 3.