Diffraction Enhanced X-ray Imaging (DEI) Benjamin Reinhart Physics 570 Final Presentation December 6 th, 2013
|
|
- Emmeline Burns
- 6 years ago
- Views:
Transcription
1 Diffraction Enhanced X-ray Imaging (DEI) Benjamin Reinhart Physics 570 Final Presentation December 6 th, 2013
2 Bullet Points of Presentation Radiography vs. Diffraction Enhanced Imaging (DEI) Basic Principles of DEI Absorption Refraction Scattering Extracting Image Data Extinction (Scatter Rejection) Refraction Scattering Applications
3 Radiography vs. DEI Detector Conventional Setup Object Monochromator X-rays Detector DEI Setup Analyzer Object Monochromator X-rays
4 Detector Conventional Setup Object Monochromator X-rays
5 Detector Conventional Setup Object Monochromator X-rays Absorption
6 Detector DEI Setup Analyzer Object Monochromator X-rays Absorption
7 Detector DEI Setup Analyzer Object Monochromator X-rays Scattering Refraction
8 Detector DEI Setup Analyzer Object Monochromator X-rays Rocking Curve What makes DEI different from conventional radiography? Intensity [Arb. units] The Analyzer Crystal used to create a rocking curve (micro-radian width) From the Rocking Curve the Principles of DEI can be extracted angle [urad] Here is how it works.
9 Detector DEI Setup Analyzer Object Monochromator X-rays Intensity [Arb. units] Rocking Curve Conventional Radiograpy uses the Recorded Intensity to get an image, variation in intensity gives a contrast. Scattering components (I, C) and Small-angle scattering (D) lead to a loss in contrast as well as spatial resolution. Refraction (R) is lost angle [urad]
10 Detector DEI Setup Analyzer Object Monochromator X-rays Rocking Curve DEI (analyzer crystal) preserves many of these components and takes advantage of them. Intensity [Arb. units] Small-angle scattering (D) is mostly eliminated due to the xstal rejecting all angles above the microradian range. Imaged objects are usually in milliradian range well above the crystal optics Refraction (R) is all that is left and can be separated angle [urad]
11 DEI there are two images taken. Each side of the rocking curve. Apparent absorption and refraction information. Intensity diffracted by analyzer crystal I(B) Darwin Width
12 Reflectivity of the analyzer crystal For small values of Δθz using Taylor Series approximation for Reflectivity of the analyzer.
13 Intensity of the Images can be calculated for the left side and right side of the rocking curve. Solving these two equations for Extinction and Refraction.
14 Intensity of the Images can be calculated for the left side and right side of the rocking curve. Solving these two equations for Refraction and Extinction. The algorithm can be applied to each pixel from both sides of the rocking curve to form the DEI images.
15 Extracting Image Data Extinction Rocking Curve Intensity [Arb. units] angle [urad] Based only on the absorption properties of the object. Refraction and Small Angle Scattering are eliminated.
16 Extracting Image Data Refraction Rocking Curve Intensity [Arb. units] angle [urad] Based only on the Refraction properties of the object. Extinction and Small Angle Scattering are eliminated.
17 Extracting Image Data Scattering Rocking Curve Intensity [Arb. units] angle [urad] Based only on the scattering properties of the object. Refraction and Extinction are eliminated.
18 Applications Mammography
19 Applications Mammography
20 The Future and Thanks Lab based machines (mammograms/children) CT Imaging with Refraction Dean Chapmann, Zhong Zhong Inventors of the method US Army Grant funding the research NSLS/DOE research location Questions?
Today s Outline - April 17, C. Segre (IIT) PHYS Spring 2018 April 17, / 22
Today s Outline - April 17, 2018 C. Segre (IIT) PHYS 570 - Spring 2018 April 17, 2018 1 / 22 Today s Outline - April 17, 2018 Diffraction enhanced imaging C. Segre (IIT) PHYS 570 - Spring 2018 April 17,
More informationDynamical Theory of X-Ray Diffraction
Dynamical Theory of X-Ray Diffraction ANDRE AUTHIER Universite P. et M. Curie, Paris OXFORD UNIVERSITY PRESS Contents I Background and basic results 1 1 Historical developments 3 1.1 Prologue 3 1.2 The
More informationInterpretation of Refraction Images in Synchrotron Based Imaging Techniques Using Growth Plate Injury Specimens in an Animal Model
Interpretation of Refraction Images in Synchrotron Based Imaging Techniques Using Growth Plate Injury Specimens in an Animal Model A Thesis Submitted to the College of Graduate Studies and Research in
More informationLIGHT SCATTERING THEORY
LIGHT SCATTERING THEORY Laser Diffraction (Static Light Scattering) When a Light beam Strikes a Particle Some of the light is: Diffracted Reflected Refracted Absorbed and Reradiated Reflected Refracted
More informationAbstract Horiba, Hironobu. 3-D Computed Tomography Using Diffraction Enhanced Imaging Modality. (Under the Direction of Professor Kuruvilla Verghese
Abstract Horiba, Hironobu. 3-D Computed Tomography Using Diffraction Enhanced Imaging Modality. (Under the Direction of Professor Kuruvilla Verghese and Professor Dale E. Sayers.) Atomic and nuclear radiation
More informationComputed tomography of x-ray index of refraction using the diffraction enhanced imaging method
Phys. Med. Biol. 45 (2000) 933 946. Printed in the UK PII: S0031-9155(00)07912-4 Computed tomography of x-ray index of refraction using the diffraction enhanced imaging method F A Dilmanian, Z Zhong, B
More informationLight. Electromagnetic wave with wave-like nature Refraction Interference Diffraction
Light Electromagnetic wave with wave-like nature Refraction Interference Diffraction Light Electromagnetic wave with wave-like nature Refraction Interference Diffraction Photons with particle-like nature
More informationIntroduction to Biomedical Imaging
Alejandro Frangi, PhD Computational Imaging Lab Department of Information & Communication Technology Pompeu Fabra University www.cilab.upf.edu X-ray Projection Imaging Computed Tomography Digital X-ray
More informationDiffraction and Interference
Diffraction and Interference Kyle Weigand, Mark Hillstrom Abstract: We measure the patterns produced by a CW laser near 650 nm passing through one and two slit apertures with a detector mounted on a linear
More informationCharacterizing x-ray mirrors in reciprocal space
Characterizing x-ray mirrors in reciprocal space Preliminary results from the NIST X-ray Optics Evaluation Double-Crystal Diffractometer D.L. Gil, D. Windover, J.P. Cline, A. Henins National Institute
More informationCrystal Quality Analysis Group
Crystal Quality Analysis Group Contents Contents 1. Overview...1 2. Measurement principles...3 2.1 Considerations related to orientation and diffraction conditions... 3 2.2 Rocking curve measurement...
More informationChapter 24. Wave Optics
Chapter 24 Wave Optics Diffraction Huygen s principle requires that the waves spread out after they pass through slits This spreading out of light from its initial line of travel is called diffraction
More informationFRESNEL LENS DIMENSIONS USING 3D PROFILOMETRY
FRESNEL LENS DIMENSIONS USING 3D PROFILOMETRY Prepared by Duanjie Li & Benjamin Mell 6 Morgan, Ste156, Irvine CA 92618 P: 949.461.9292 F: 949.461.9232 nanovea.com Today's standard for tomorrow's materials.
More informationPhase-Contrast Imaging and Tomography at 60 kev using a Conventional X-ray Tube
Phase-Contrast Imaging and Tomography at 60 kev using a Conventional X-ray Tube T. Donath* a, F. Pfeiffer a,b, O. Bunk a, W. Groot a, M. Bednarzik a, C. Grünzweig a, E. Hempel c, S. Popescu c, M. Hoheisel
More informationImage Acquisition Systems
Image Acquisition Systems Goals and Terminology Conventional Radiography Axial Tomography Computer Axial Tomography (CAT) Magnetic Resonance Imaging (MRI) PET, SPECT Ultrasound Microscopy Imaging ITCS
More informationAdvanced Graphics. Path Tracing and Photon Mapping Part 2. Path Tracing and Photon Mapping
Advanced Graphics Path Tracing and Photon Mapping Part 2 Path Tracing and Photon Mapping Importance Sampling Combine importance sampling techniques Reflectance function (diffuse + specular) Light source
More informationX-rays are electro-magnetic radiation
X-rays are electro-magnetic radiation Just like visible light, X-rays are waves - cos[ 2π ( x / λ ft)] X-rays travel at the speed of light (c) Quantum Mechanics gives the energy of an X-ray photon c =
More informationTracePro Stray Light Simulation
TracePro Stray Light Simulation What Is Stray Light? A more descriptive term for stray light is unwanted light. In an optical imaging system, stray light is caused by light from a bright source shining
More informationHigh spatial resolution measurement of volume holographic gratings
High spatial resolution measurement of volume holographic gratings Gregory J. Steckman, Frank Havermeyer Ondax, Inc., 8 E. Duarte Rd., Monrovia, CA, USA 9116 ABSTRACT The conventional approach for measuring
More informationA computed tomography implementation of multiple-image radiography
A computed tomography implementation of multiple-image radiography Jovan G. Brankov Department of Electrical and Computer Engineering, Illinois Institute of Technology, Chicago, Illinois 60616 Miles N.
More informationThe Importance of Refractive Index When using Laser Diffraction
The Importance of Refractive Index When using Laser Diffraction Mark Bumiller mark.bumiller@horiba.com Fraunhofer Approximation Mie Theory RI 1.60 0.0i, in water, RI 1.33 Mie vs. Fraunhofer 1.E+05 1.E+04
More informationRietveld refinements collection strategies!
Rietveld refinements collection strategies! Luca Lutterotti! Department of Materials Engineering and Industrial Technologies! University of Trento - Italy! Quality of the experiment! A good refinement,
More informationIntroduction. Experiment A: Snell s Law. Physics 1CL REFLECTION AND REFRACTION OF LIGHT Summer Session II 2010
Introduction This laboratory is a quantitative investigation of the reflection and refraction of light off optical interfaces. An optical interface is a boundary between two transparent media of different
More informationTHREE-DIMENSIONAL MAPPING OF FATIGUE CRACK POSITION VIA A NOVEL X-RAY PHASE CONTRAST APPROACH
Copyright JCPDS - International Centre for Diffraction Data 2003, Advances in X-ray Analysis, Volume 46. 314 THREE-DIMENSIONAL MAPPING OF FATIGUE CRACK POSITION VIA A NOVEL X-RAY PHASE CONTRAST APPROACH
More informationGG450 4/5/2010. Today s material comes from p and in the text book. Please read and understand all of this material!
GG450 April 6, 2010 Seismic Reflection I Today s material comes from p. 32-33 and 81-116 in the text book. Please read and understand all of this material! Back to seismic waves Last week we talked about
More informationCoupling of surface roughness to the performance of computer-generated holograms
Coupling of surface roughness to the performance of computer-generated holograms Ping Zhou* and Jim Burge College of Optical Sciences, University of Arizona, Tucson, Arizona 85721, USA *Corresponding author:
More informationTEM Imaging and Dynamical Scattering
TEM Imaging and Dynamical Scattering Duncan Alexander EPFL-CIME 1 Aspects of TEM imaging Objective lens focus Objective lens astigmatism Image delocalization Dynamical scattering 2-beam theory Thickness
More informationRSoft Product Applications
RSoft Product Applications Complete design solutions for photonic components, circuits and systems synopsys.com/optical-solutions/rsoft RSoft Photonic Design Software Applications Synopsys RSoft products
More informationCHAPTER 26 INTERFERENCE AND DIFFRACTION
CHAPTER 26 INTERFERENCE AND DIFFRACTION INTERFERENCE CONSTRUCTIVE DESTRUCTIVE YOUNG S EXPERIMENT THIN FILMS NEWTON S RINGS DIFFRACTION SINGLE SLIT MULTIPLE SLITS RESOLVING POWER 1 IN PHASE 180 0 OUT OF
More informationPHYSICS 116 POLARIZATION AND LIGHT MEASUREMENTS
Name Date Lab Time Lab TA PHYSICS 116 POLARIZATION AND LIGHT MEASUREMENTS I. POLARIZATION Natural unpolarized light is made up of waves vibrating in all directions. When a beam of unpolarized light is
More informationEnergy resolved X-ray diffraction Cl. J.Kosanetzky, G.Harding, U.Neitzel
Proc. Of SPIE Vol 0626, Application of Optical Instrumentation in Medicine XIV and Picture Archiving and Communication Systems(PACS IV) for Medical Applications IV, ed. S J Dwyer/R H Schneider (Jan 1986)
More informationLenses lens equation (for a thin lens) = (η η ) f r 1 r 2
Lenses lens equation (for a thin lens) 1 1 1 ---- = (η η ) ------ - ------ f r 1 r 2 Where object o f = focal length η = refractive index of lens material η = refractive index of adjacent material r 1
More informationRaycasting. Ronald Peikert SciVis Raycasting 3-1
Raycasting Ronald Peikert SciVis 2007 - Raycasting 3-1 Direct volume rendering Volume rendering (sometimes called direct volume rendering) stands for methods that generate images directly from 3D scalar
More informationLaboratory 6: Light and the Laser
Laboratory 6: Light and the Laser WARNING NEVER LOOK DIRECTLY AT LASER LIGHT Index of Refraction: Snell's Law 1. Read the section on physical optics in some introductory physics text. 2. Set the semicircular
More informationInterference and Diffraction of Light
Name Date Time to Complete h m Partner Course/ Section / Grade Interference and Diffraction of Light Reflection by mirrors and refraction by prisms and lenses can be analyzed using the simple ray model
More informationSimple Spatial Domain Filtering
Simple Spatial Domain Filtering Binary Filters Non-phase-preserving Fourier transform planes Simple phase-step filters (for phase-contrast imaging) Amplitude inverse filters, related to apodization Contrast
More informationDUAL energy X-ray radiography [1] can be used to separate
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 1, FEBRUARY 2006 133 A Scatter Correction Using Thickness Iteration in Dual-Energy Radiography S. K. Ahn, G. Cho, and H. Jeon Abstract In dual-energy
More informationMultiple-image radiography
INSTITUTE OF PHYSICS PUBLISHING Phys. Med. Biol. 48 (2003) 3875 3895 PHYSICS IN MEDICINE AND BIOLOGY PII: S0031-9155(03)65305-4 Multiple-image radiography Miles N Wernick 1,4,OliverWirjadi 1,6,Dean Chapman
More information8/3/2016. Outline. The EPID Strikes Back: Future EPID Technology and Applications. Active Matrix Flat-Panel Imagers (AMFPIs)
8//6 The EPID Strikes Back: Future EPID Technology and Applications Larry E. Antonuk Department of Radiation Oncology University of Michigan, Ann Arbor Acknowledgements: Youcef El-Mohri, Qihua Zhao (U.
More informationMonte Carlo Method for Solving Inverse Problems of Radiation Transfer
INVERSE AND ILL-POSED PROBLEMS SERIES Monte Carlo Method for Solving Inverse Problems of Radiation Transfer V.S.Antyufeev. ///VSP/// UTRECHT BOSTON KÖLN TOKYO 2000 Contents Chapter 1. Monte Carlo modifications
More informationActivity 9.1 The Diffraction Grating
PHY385H1F Introductory Optics Practicals Day 9 Diffraction November 29, 2010 Please work in a team of 3 or 4 students. All members should find a way to contribute. Two members have a particular role, and
More informationExperiment 6. Snell s Law. Use Snell s Law to determine the index of refraction of Lucite.
Experiment 6 Snell s Law 6.1 Objectives Use Snell s Law to determine the index of refraction of Lucite. Observe total internal reflection and calculate the critical angle. Explain the basis of how optical
More informationSpectrophotometric Methods of Refractive Indices Measurement
Application Note Glass, ceramics, optics Spectrophotometric Methods of Refractive Indices Measurement Measuring the refractive index of single crystal optical materials using two methods Authors N.S. Kozlova
More informationUNDERSTANDING CALCULATION LEVEL AND ITERATIVE DECONVOLUTION
UNDERSTANDING CALCULATION LEVEL AND ITERATIVE DECONVOLUTION Laser diffraction particle size analyzers use advanced mathematical algorithms to convert a measured scattered light intensity distribution into
More informationChapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena
Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics
More informationUniversity Physics (Prof. David Flory) Chapt_37 Monday, August 06, 2007
Name: Date: 1. If we increase the wavelength of the light used to form a double-slit diffraction pattern: A) the width of the central diffraction peak increases and the number of bright fringes within
More informationTHE EFFECT OF SURFACE ROUGHNESS OF CSI(TL) MICRO-COLUMNS ON THE RESOLUTION OF THE X-RAY IMAGE; OPTICAL SIMULATION STUDY
PAPER THE EFFECT OF SURFACE ROUGHNESS OF CSI(TL) MICRO-COLUMNS ON THE RESOLUTION OF THE X-RAY IMAGE; OPTICAL SIMULATION STUDY HYUNKI KIM, JUN HYUNG BAE, BO KYUNG CHA, HOSANG JEON, JONG YUL KIM, CHAN KYU
More informationLiquid Crystal Displays
Liquid Crystal Displays Irma Alejandra Nicholls College of Optical Sciences University of Arizona, Tucson, Arizona U.S.A. 85721 iramirez@email.arizona.edu Abstract This document is a brief discussion of
More informationSupplementary materials of Multispectral imaging using a single bucket detector
Supplementary materials of Multispectral imaging using a single bucket detector Liheng Bian 1, Jinli Suo 1,, Guohai Situ 2, Ziwei Li 1, Jingtao Fan 1, Feng Chen 1 and Qionghai Dai 1 1 Department of Automation,
More informationOriginal grey level r Fig.1
Point Processing: In point processing, we work with single pixels i.e. T is 1 x 1 operator. It means that the new value f(x, y) depends on the operator T and the present f(x, y). Some of the common examples
More informationAddressing High Precision Automated Optical Inspection Challenges with Unique 3D Technology Solution
Addressing High Precision Automated Optical Inspection Challenges with Unique 3D Technology Solution John Hoffman CyberOptics Corporation jhoffman@cyberoptics.com Outline/Agenda Phase Profilometry SMT
More information12/7/2012. Biomolecular structure. Diffraction, X-ray crystallography, light- and electron microscopy. CD spectroscopy, mass spectrometry
phase difference at a given distance constructive/destructive interference Biomolecular structure. Diffraction, X-ray crystallography, light- and electron microscopy. CD spectroscopy, mass spectrometry
More informationRadiography and Tomography Lab 2: Computing Radiographs
Radiography and Tomography Lab 2: Computing Radiographs An Abbreviated View of Radiography Transmission Radiography is the process of measuring and recording changes in a high-energy particle beam (X-rays,
More information1/12/2009. Image Elements (Pixels) Image Elements (Pixels) Digital Image. Digital Image =...
PAM3012 Digital Image Processing for Radiographers Image Sampling & Quantization In this lecture Definitions of Spatial l & Gray-level l resolution Perceived Image Quality & Resolution Aliasing & Moire
More informationStress and Texture by XRD Bob He, Bruker AXS
Stress and Texture by XRD Bob He, Bruker AXS Intensity Conventional X-ray Diffractometer Divergence slit Antiscatter slit Monochromator Bragg-Brentano Geometry. Scanning over range to collect XRD pattern.
More informationOPTI-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 informationBME I5000: Biomedical Imaging
1 Lucas Parra, CCNY BME I5000: Biomedical Imaging Lecture 4 Computed Tomography Lucas C. Parra, parra@ccny.cuny.edu some slides inspired by lecture notes of Andreas H. Hilscher at Columbia University.
More informationCh. 4 Physical Principles of CT
Ch. 4 Physical Principles of CT CLRS 408: Intro to CT Department of Radiation Sciences Review: Why CT? Solution for radiography/tomography limitations Superimposition of structures Distinguishing between
More informationCHEM-E5225 :Electron Microscopy Imaging I
CHEM-E5225 :Electron Microscopy Imaging I 2018.11 Yanling Ge Outline Amplitude Contrast Phase Contrast Images Thickness and Bending Effects Amplitude Contrast Amplitude phase TEM STEM Incoherent elastic
More informationPhysics 202, Lecture 23
Physics 202, Lecture 23 Today s Topics Lights and Laws of Geometric Optics Nature of Light Reflection and Refraction Law of Reflection Law of Refraction Index of Reflection, Snell s Law Total Internal
More informationRICH12 Update: Simulations
RICH12 Update: Simulations Material Properties 1 p.e. Resolution Np.e.Counting N. Baltzell Argonne National Laboratory CLAS12 Workshop February 22, 2012 Aerogel Scattering & Absorption Lengths Material
More informationSimple Spectrograph. grating. slit. camera lens. collimator. primary
Simple Spectrograph slit grating camera lens collimator primary Notes: 1) For ease of sketching, this shows a transmissive system (refracting telescope, transmission grating). Most telescopes use a reflecting
More information45 µm polystyrene bead embedded in scattering tissue phantom. (a,b) raw images under oblique
Phase gradient microscopy in thick tissue with oblique back-illumination Tim N Ford, Kengyeh K Chu & Jerome Mertz Supplementary Figure 1: Comparison of added versus subtracted raw OBM images 45 µm polystyrene
More informationdiffraction patterns obtained with convergent electron beams yield more information than patterns obtained with parallel electron beams:
CBED-Patterns Principle of CBED diffraction patterns obtained with convergent electron beams yield more information than patterns obtained with parallel electron beams: specimen thickness more precise
More informationdq dt I = Irradiance or Light Intensity is Flux Φ per area A (W/m 2 ) Φ =
Radiometry (From Intro to Optics, Pedrotti -4) Radiometry is measurement of Emag radiation (light) Consider a small spherical source Total energy radiating from the body over some time is Q total Radiant
More informationTwo pixel computer generated hologram using a zero twist nematic liquid crystal spatial light modulator
Two pixel computer generated hologram using a zero twist nematic liquid crystal spatial light modulator Philip M. Birch, Rupert Young, David Budgett, Chris Chatwin School of Engineering, University of
More informationPhysics 309 Lab 3. where the small angle approximation has been used. This pattern has maxima at. Y Max. n L /d (2)
Physics 309 Lab 3 Introduction This will be a lab whose purpose is to give you some hands-on experience with optical interference and diffraction, using small green diode lasers as the light sources. Each
More informationChapter 24. Wave Optics
Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics
More informationPlane Wave Imaging Using Phased Array Arno Volker 1
11th European Conference on Non-Destructive Testing (ECNDT 2014), October 6-10, 2014, Prague, Czech Republic More Info at Open Access Database www.ndt.net/?id=16409 Plane Wave Imaging Using Phased Array
More informationMedical Image Processing: Image Reconstruction and 3D Renderings
Medical Image Processing: Image Reconstruction and 3D Renderings 김보형 서울대학교컴퓨터공학부 Computer Graphics and Image Processing Lab. 2011. 3. 23 1 Computer Graphics & Image Processing Computer Graphics : Create,
More informationRay Optics. Lecture 23. Chapter 23. Physics II. Course website:
Lecture 23 Chapter 23 Physics II Ray Optics Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsii Let s finish talking about a diffraction grating Diffraction Grating Let s improve (more
More informationDigital Scatter Removal in Mammography to enable Patient Dose Reduction
Digital Scatter Removal in Mammography to enable Patient Dose Reduction Mary Cocker Radiation Physics and Protection Oxford University Hospitals NHS Trust Chris Tromans, Mike Brady University of Oxford
More informationChapter 38. Diffraction Patterns and Polarization
Chapter 38 Diffraction Patterns and Polarization Diffraction Light of wavelength comparable to or larger than the width of a slit spreads out in all forward directions upon passing through the slit This
More informationIntroduction to Computer Vision. Introduction CMPSCI 591A/691A CMPSCI 570/670. Image Formation
Introduction CMPSCI 591A/691A CMPSCI 570/670 Image Formation Lecture Outline Light and Optics Pinhole camera model Perspective projection Thin lens model Fundamental equation Distortion: spherical & chromatic
More informationEffective Medium Theory, Rough Surfaces, and Moth s Eyes
Effective Medium Theory, Rough Surfaces, and Moth s Eyes R. Steven Turley, David Allred, Anthony Willey, Joseph Muhlestein, and Zephne Larsen Brigham Young University, Provo, Utah Abstract Optics in the
More informationChapter 35 &36 Physical Optics
Chapter 35 &36 Physical Optics Physical Optics Phase Difference & Coherence Thin Film Interference 2-Slit Interference Single Slit Interference Diffraction Patterns Diffraction Grating Diffraction & Resolution
More informationReflection and Refraction of Light
Name: Date: PC1222 Fundamentals of Physics II Reflection and Refraction of Light 5 Laboratory Worksheet Part A: Law of Reflection Angle of Incidence θ i Angle of Reflection θ r Data Table 1: Reflection
More informationImage Processing
Image Processing 159.731 Canny Edge Detection Report Syed Irfanullah, Azeezullah 00297844 Danh Anh Huynh 02136047 1 Canny Edge Detection INTRODUCTION Edges Edges characterize boundaries and are therefore
More informationSUPPLEMENTARY INFORMATION
doi:10.1038/nature09750 "#$%&'($)* #+"%%*,-.* /&01"2*$3* &)(4&"* 2"3%"5'($)#* 6&%'(7%(5('8* 9$07%"'": )"##*,;.*
More informationPart 1: Plane Mirrors!
Algodoo Optics Part 1: Plane Mirrors This activity will model, using Algodoo, the mirror lab experiment from class. With a physical model, students are asked to look into the mirror from two different
More informationLC-1: Interference and Diffraction
Your TA will use this sheet to score your lab. It is to be turned in at the end of lab. You must use complete sentences and clearly explain your reasoning to receive full credit. The lab setup has been
More informationLight and Sound. Wave Behavior and Interactions
Light and Sound Wave Behavior and Interactions How do light/sound waves interact with matter? WORD Definition Example Picture REFLECTED REFRACTED is the change in direction of a wave when it changes speed
More informationOPSE FINAL EXAM Fall CLOSED BOOK. Two pages (front/back of both pages) of equations are allowed.
CLOSED BOOK. Two pages (front/back of both pages) of equations are allowed. YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT. ALL NUMERICAL ANSERS MUST HAVE UNITS INDICATED.
More informationX PERT DATA COLLECTOR. Quick Start Guide
X PERT DATA COLLECTOR Quick Start Guide X Pert Data Collector Quick Start Guide EDITION NOTICE: Sixth Edition, January 2006. This is the sixth edition of this publication, it is intended for use with
More informationIntroduction to Microeletromechanical Systems (MEMS) Lecture 8 Topics. MEMS Overview
Introduction to Microeletromechanical Systems (MEMS) Lecture 8 Topics MicroOptoElectroMechanical Systems (MOEMS) Scanning D Micromirrors TI Digital Light Projection Device Basic Optics: Refraction and
More informationChapter 24. Wave Optics. Wave Optics. The wave nature of light is needed to explain various phenomena
Chapter 24 Wave Optics Wave Optics The wave nature of light is needed to explain various phenomena Interference Diffraction Polarization The particle nature of light was the basis for ray (geometric) optics
More informationRefraction and Polarization of Light
Chapter 9 Refraction and Polarization of Light Name: Lab Partner: Section: 9.1 Purpose The purpose of this experiment is to demonstrate several consequences of the fact that materials have di erent indexes
More informationX-Ray Refraction Topography and Computed Tomography for NDE of Lightweight Materials
ECNDT 2006 - Tu.3.5.3 X-Ray Refraction Topography and Computed Tomography for NDE of Lightweight Materials Bernd R. MÜLLER, Axel LANGE, Michael HARWARDT, Manfred P. HENTSCHEL, Bernhard ILLERHAUS, Jürgen
More informationSTEP HEIGHT MEASUREMENT OF PRINTED ELECTRODES USING 3D PROFILOMETRY
STEP HEIGHT MEASUREMENT OF PRINTED ELECTRODES USING D PROFILOMETRY Prepared by Andrea Herrmann Morgan, Ste, Irvine CA 98 P: 99..99 F: 99..9 nanovea.com Today's standard for tomorrow's materials. NANOVEA
More informationPHY 171 Lecture 6 (January 18, 2012)
PHY 171 Lecture 6 (January 18, 2012) Light Throughout most of the next 2 weeks, we will be concerned with the wave properties of light, and phenomena based on them (interference & diffraction). Light also
More informationMoscow-Bavarian Joint Advanced Student School 2006 / Medical Imaging Principles of Computerized Tomographic Imaging and Cone-Beam Reconstruction
Line Integrals Line integrals represent the integral of some parameter of the object along the line (e.g. attenuation of x-rays) Object: f(x,y) Line: x cosθ + y sinθ = t Line integral / Radon transform:
More informationEngineered Diffusers Intensity vs Irradiance
Engineered Diffusers Intensity vs Irradiance Engineered Diffusers are specified by their divergence angle and intensity profile. The divergence angle usually is given as the width of the intensity distribution
More informationGaussian Beam Calculator for Creating Coherent Sources
Gaussian Beam Calculator for Creating Coherent Sources INTRODUCTION Coherent sources are represented in FRED using a superposition of Gaussian beamlets. The ray grid spacing of the source is used to determine
More informationExercise 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 informationX-ray Powder Diffraction
X-ray Powder Diffraction Chemistry 754 Solid State Chemistry Lecture #8 April 15, 2004 Single Crystal Diffraction Diffracted Beam Incident Beam Powder Diffraction Diffracted Beam Incident Beam In powder
More informationQuick Start Guide. X Pert Data Collector
Quick Start Guide X Pert Data Collector X PERT DATA COLLECTOR QUICK START GUIDE EDITION NOTICE: Fifth Edition, October 2004. This is the fifth edition of this publication, it is intended for use with
More informationACCURATE TEXTURE MEASUREMENTS ON THIN FILMS USING A POWDER X-RAY DIFFRACTOMETER
ACCURATE TEXTURE MEASUREMENTS ON THIN FILMS USING A POWDER X-RAY DIFFRACTOMETER MARK D. VAUDIN NIST, Gaithersburg, MD, USA. Abstract A fast and accurate method that uses a conventional powder x-ray diffractometer
More informationInspection Technology Europe BV Allied NDT Engineers
What is Gloss? Gloss is an optical phenomenon caused when evaluating the appearance of a surface. The evaluation of gloss describes the capacity of a surface to reflect directed light. Why is gloss measured?
More informationISO INTERNATIONAL STANDARD. Particle size analysis Laser diffraction methods. Analyse granulométrique Méthodes par diffraction laser
INTERNATIONAL STANDARD ISO 13320 First edition 2009-10-01 Corrected version 2009-12-01 Particle size analysis Laser diffraction methods Analyse granulométrique Méthodes par diffraction laser Reference
More informationDESIGNER S NOTEBOOK Proximity Detection and Link Budget By Tom Dunn July 2011
INTELLIGENT OPTO SENSOR Number 38 DESIGNER S NOTEBOOK Proximity Detection and Link Budget By Tom Dunn July 2011 Overview TAOS proximity sensors operate by flashing an infrared (IR) light towards a surface
More information