Large-Format Geiger-Mode Avalanche Photodiode Arrays and Readout Circuits Brian F
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Al0.48 In0.52 As Superlattice Avalanche Photodiodes On
www.nature.com/scientificreports OPEN Engineering of impact ionization characteristics in In0.53Ga0.47As/ Al0.48In0.52As superlattice avalanche photodiodes on InP substrate S. Lee1, M. Winslow2, C. H. Grein2, S. H. Kodati1, A. H. Jones3, D. R. Fink1, P Das4, M. M. Hayat4, T. J. Ronningen1, J. C. Campbell3 & S. Krishna1* We report on engineering impact ionization characteristics of In0.53Ga0.47As/Al0.48In0.52As superlattice avalanche photodiodes (InGaAs/AlInAs SL APDs) on InP substrate to design and demonstrate an APD with low k-value. We design InGaAs/AlInAs SL APDs with three diferent SL periods (4 ML, 6 ML, and 8 ML) to achieve the same composition as Al0.4Ga0.07In0.53As quaternary random alloy (RA). The simulated results of an RA and the three SLs predict that the SLs have lower k-values than the RA because the electrons can readily reach their threshold energy for impact ionization while the holes experience the multiple valence minibands scattering. The shorter period of SL shows the lower k-value. To support the theoretical prediction, the designed 6 ML and 8 ML SLs are experimentally demonstrated. The 8 ML SL shows k-value of 0.22, which is lower than the k-value of the RA. The 6 ML SL exhibits even lower k-value than the 8 ML SL, indicating that the shorter period of the SL, the lower k-value as predicted. This work is a theoretical modeling and experimental demonstration of engineering avalanche characteristics in InGaAs/AlInAs SLs and would assist one to design the SLs with improved performance for various SWIR APD application. -
The Effective Application of Digital Printing Techniques for Fine Artists in the South African Context
The effective application of digital printing techniques for fine artists in the South African context. a Dissertation BY Susan Louise Giloi (NH Dip: Photography) Submitted in partial compliance with the requirements for the Degree Magister Technologiae in Photography in the Department of Photography, Faculty of Art and Design. PORT ELIZABETH TECHNIKON November 1999 PROMOTERS Prof. N.P.L. Allen M.F.A. D.Phil. Laur Tech Mr S.C. Strooh N Dip: Photography DEDICATION To my family who gave me the opportunity to do this. To Prof. Nicholas Allen and Mr. Steven Strooh for their help and inspiration. ii ACKNOWLEDGEMENTS My thanks to all the individuals and companies that helped me. Ashley Bowers, Tone Graphics Billy Whitehair, Printing Products Bonny Lhotka Bruce Cadle, Port Elizabeth Technikon Carol Van Zyl, Vaal Triangle Technikon Cleone Cull, Port Elizabeth Technikon Colleen Bate, Digital Imaging and Publishing Dean Johnstone, Square One Dianna Wall, Museum Africa Dorothy Krause Edwin Taylor, Beith Digital Eileen Fritsch, Big Picture Magazine Ethna Frankenfeld, Port Elizabeth Technikon Eugene Pienaar, Port Elizabeth Technikon Gavin Van Rensburg, Kemtek Geoff Black, Cyber Distributors Glen Meyer, Port Elizabeth Technikon Hank Van Der Water, Xerox E.C. Ian de Vega, Port Elizabeth Technikon Ian Marley, Vaal Triangle Technikon Ian White, John Cook University Inge Economou, Port Elizabeth Technikon Isabel Lubbe, Vaal Triangle Technikon Isabel Smit, Yeltech Jenny Ord, Port Elizabeth Technikon John Clarke, JFC Clarke Studio John Otsuki, Capitol Color Keith Solomon, First Graphics Laraine Bekker, Port Elizabteh Technikon Lisle Nel, Port Elizabeth Technikon Magda Bosch, Port Elizabteh Technikon Mary Duker, Port Elizabeth Technikon Mike Swanepoel, Port Elizabeth Technikon Nick Hand, Nexus Nolan Weight, Stonehouse Graphics Peter Thome, Agfa SA Robin Mowatt, QMS Ronald Henry, Omni Graphics Ros Streak, City Graphics Russell Williams, Teltron Steve Majewski Thinus Mathee, Vaal Triangle Technikon iii Tilla Jordaan, Xerox SA Tony Davidson, Outdoor Advertising Association of S.A. -
Leds As Single-Photon Avalanche Photodiodes by Jonathan Newport, American University
LEDs as Single-Photon Avalanche Photodiodes by Jonathan Newport, American University Lab Objectives: Use a photon detector to illustrate properties of random counting experiments. Use limiting probability distributions to perform statistical analysis on a physical system. Plot histograms. Condition a detector’s signal for further electronic processing. Use a breadboard, power supply and oscilloscope to construct a circuit and make measurements. Learn about semiconductor device physics. Reading: Taylor 3.2 – The Square-Root Rule for a Counting Experiment pp. 48-49 Taylor 5.1-5.3 – Histograms and the Normal Distribution pp. 121-135 Taylor Ch. 11 – The Poisson Distribution pp. 245-254 Taylor Problem 5.6 – The Exponential Distribution p. 155 Experiment #1: Lighting an LED A Light-Emitting Diode is a non-linear circuit element that can produce a controlled amount of light. The AND113R datasheet shows that the luminous intensity is proportional to the current flowing through the LED. As illustrated in the IV curve shown below, the current flowing through the diode is in turn proportional to the voltage across the diode. Diodes behave like a one-way valve for current. When the voltage on the Anode is more positive than the voltage on the Cathode, then the diode is said to be in Forward Bias. As the voltage across the diode increases, the current through the diode increases dramatically. The heat generated by this current can easily destroy the device. It is therefore wise to install a current-limiting resistor in series with the diode to prevent thermal runaway. When the voltage on the Cathode is more positive than the voltage on the Anode, the diode is said to be in Reverse Bias. -
Flat-Panel Imaging Arrays for Digital Radiography
Outline Flat-Panel Imaging Arrays • Market and clinical challenges for digital radiography for Digital Radiography • Passive pixel amorphous silicon imaging arrays • Active pixel amorphous silicon imaging arrays Timothy Tredwell, Jeff Chang, Jackson Lai, Greg Heiler, Mark Shafer, John Yorkston Carestream Health, Inc., Rochester, NY 14615, USA • Active pixel LTPS imaging arrays Jin Jang, Jae Won Choi, Jae Ik Kim, Seung Hyun Park, Jun Hyuk Cheon, Sauabh Saxena, Won Kyu Lee • Silicon-on-glass circuits for future active pixel imaging Advanced Display Research Center, Kyung Hee University, Seoul, Korea arrays Arokia Nathan London Center for Nanotechnology, University College, London Eric Mozdy, Carlo Kosik Williams, Jeffery Cites, Chuan Che Wang Corning Incorporated, Sullivan Park, Corning, NY 14831, USA 2 DR: “Digital” Radiography DR: 1 step acquisition with electrical “scanning” “Flat panel” and CCD based technology (introduced ~1995) (Courtesy Imaging Dynamics Corp.) 3 4 Two-Dimensional Projection Radiography The Market Outlook for DR: Rapid Growth World’s Population is Aging • Still most common exam • >1.5 x 10 9 exams per year • Chest imaging most common 1999 2050 Procedural Volume Trends • An aging population: 2,500 • By 2050, over 25% of the population in North America, Europe, China 2,000 Nuc Med and Australia will be over 60 ULtrasound • For every 1 time a 20-year-old visits a doctor … 1,500 MR …a 60-year-old visits a doctor 26 times 1,000 CT Digital X-ray • Rising incomes in Asia and Latin America will accelerate demand Procedures (Ms) Procedures 500 Analog x-ray • Emerging economies could go direct to digital - • Cost must be low – significant market opportunity 2001 2002 2003 2004 2005 2006 2007 2008 5 Source: WHO, World Bank 6 Anatomical Noise Anatomical Noise in Projection Radiography 3-Dim 2-Dim &KHVW5DGLRJUDSK 0DPPRJUDSK\ • 3 dim. -
Thermionic and Gaseous State Diodes
THERMIONIC AND GASEOUS STATE DIODES Thermionic and gaseous state (vacuum tube) diodes Thermionic diodes are thermionic-valve devices (also known as vacuum tubes, tubes, or valves), which are arrangements of electrodes surrounded by a vacuum within a glass envelope. Early examples were fairly similar in appearance to incandescent light bulbs. In thermionic valve diodes, a current through the heater filament indirectly heats the cathode, another internal electrode treated with a mixture of barium and strontium oxides, which are oxides of alkaline earth metals; these substances are chosen because they have a small work function. (Some valves use direct heating, in which a tungsten filament acts as both heater and cathode.) The heat causes thermionic emission of electrons into the vacuum. In forward operation, a surrounding metal electrode called the anode is positively charged so that it electrostatically attracts the emitted electrons. However, electrons are not easily released from the unheated anode surface when the voltage polarity is reversed. Hence, any reverse flow is negligible. For much of the 20th century, thermionic valve diodes were used in analog signal applications, and as rectifiers in many power supplies. Today, valve diodes are only used in niche applications such as rectifiers in electric guitar and high-end audio amplifiers as well as specialized high-voltage equipment. Semiconductor diodes A modern semiconductor diode is made of a crystal of semiconductor like silicon that has impurities added to it to create a region on one side that contains negative charge carriers (electrons), called n-type semiconductor, and a region on the other side that contains positive charge carriers (holes), called p-type semiconductor. -
CHAPTER 11 HPD (Hybrid Photo-Detector)
CHAPTER 11 HPD (Hybrid Photo-Detector) HPD (Hybrid Photo-Detector) is a completely new photomultiplier tube that incorporates a semiconductor element in an evacuated elec- tron tube. In HPD operation, photoelectrons emitted from the photo- cathode are accelerated to directly strike the semiconductor where their numbers are increased. Features offered by the HPD are extremely little fluctuation during the multiplication, high electron resolution, and excellent stability. © 2007 HAMAMATSU PHOTONICS K. K. 210 CHAPTER 11 HPD (Hybrid Photo-Detector) 11.1 Operating Principle of HPDs As shown in Figure 11-1, an HPD consists of a photocathode for converting light into photoelectrons and a semiconductor element (avalanche diode or AD) which is the target for "electron bombardment" by photo- electrons. The HPD operates on the following principle: when light enters the photocathode, photoelectrons are emitted according to the amount of light; these photoelectrons are accelerated by a high-intensity electric field of a few kilovolts to several dozen kilovolts applied to the photocathode; they are then bombarded onto the target semiconductor where electron-hole pairs are generated according to the incident energy of the photoelectrons. This is called "electron bombardment gain". A typical relation between this electron bom- bardment gain and the photocathode supply voltage is plotted in Figure 11-2. In principle, this electron bom- bardment gain is proportional to the photocathode supply voltage. However, there is actually a loss of energy in the electron bombardment due to the insensitive surface layer of the semiconductor, so their proportional relation does not hold at a low voltage. In Figure 11-2, the voltage at a point on the voltage axis (horizontal axis) where the dotted line intersects is called the threshold voltage [Vth]. -
Digital and Advanced Imaging Equipment
CHAPTER 9 Digital and Advanced Imaging Equipment KEY TERMS active matrix array direct-to-digital radiographic systems photostimulated luminescence amorphous dual-energy x-ray absorptiometry picture archiving and communication analog-to-digital converter F-center system aspect ratio fill factor preprocessing cinefluorography frame rate postprocessing computed radiography image contrast refresh rate detective quantum efficiency image enhancement special procedures laboratory Digital Imaging and Communications image management and specular reflection in Medicine group communication system teleradiology digital fluoroscopy image restoration thin-film transistor digital radiography interpolation window level digital subtraction angiography liquid crystal display window width digital x-ray radiogrammetry Nyquist frequency OBJECTIVES At the completion of this chapter the reader should be able to do the following: • Describe the basic methods of obtaining digital cathode-ray tube cameras, videotape and videodisc radiographs recorders, and cinefluorographic equipment and discuss • State the advantages and disadvantages of digital the quality control procedures for each radiography versus conventional film/screen • Describe the various types of electronic display devices radiography and discuss the applicable quality control procedures • Discuss the quality control procedures for evaluating • Explain the basic image archiving and management digital radiographic systems networks and discuss the applicable quality control • Describe the basic methods -
Avalanche Diode Detector Unit
A large area avalanche photodiode detector system with USB interface 1. Introduction When measuring low light levels, a vacuum tube photomultiplier tube or some form of solid-state detector which relies on multiplication (e.g. Avalanche diode, Geiger avalanche diode, silicon photomultiplier) is normally used. Vacuum tube photomultipliers have the advantage that a large photosensitive area is available, in contrast to most solid-state devices, which, in general, allow detection over a small area. Avalanche photodiodes make excellent detectors, and here we describe a detector assembly developed around a large area device, 10 mm diameter. This detector unit is designed to detect low light levels and is based around a detector module, commercially available from AP Technology, (www.advancedphotonix.com) part# 197-70-74-661. The detector module is supplied as just that, a small box with flying leads, requiring appropriate low voltage dc power supplies. It does include a thermoelectric cooler and the avalanche diode’s high voltage bias supply. Here we describe how this module was integrated in a photo-detection subsystem, powered from the mains and controlled either from an internal potentiometer or through a computer interface. The completed unit can operate as a stand-alone, manually adjusted unit and powered from a +5V / 2.5A power supply, providing an analogue output in the range 0 to +1V into a 50 Ω (or greater) load over a typical 10 MHz bandwidth. It can also operate as a USB-controlled device, where the detector gain can be remotely set and where output readings and operating conditions can be monitored. -
Overview of Digital Detector Technology
Overview of Digital Detector Technology J. Anthony Seibert, Ph.D. Department of Radiology University of California, Davis Disclosure • Member (uncompensated) – Barco-Voxar Medical Advisory Board – ALARA (CR manufacturer) Advisory Board Learning Objectives • Describe digital versus screen-film acquisition • Introduce digital detector technologies • Compare cassette and cassette-less operation in terms of resolution, efficiency, noise • Describe new acquisition & processing techniques • Discuss PACS/RIS interfaces and features 1 Conventional screen/film detector 1. Acquisition, Display, Archiving Transmitted x-rays through patient Exposed film Film processor Developer Fixer Wash Dry Gray Scale encoded on Film Intensifying Screens film x-rays → light Digital x-ray detector 2. Display Digital Pixel Digital to Analog 1. Acquisition Matrix Conversion Transmitted x-rays through patient Digital processing Analog to Digital Conversion Charge X-ray converter collection x-rays → electrons device 3. Archiving Analog versus Digital Spatial Resolution MTF of pixel aperture (DEL) 1 100 µm 0.8 0.6 200 µm 1000 µm 0.4 Modulation 0.2 0 01234567891011 Frequency (lp/mm) Sampling Detector Pitch Element, “DEL” 2 Characteristic Curve: Response of screen/film vs. digital detectors 5 Useless 4 10,000 Film-screen (400 speed) Digital 3 1,000 Overexposed Useless 2 100 Correctly exposed 1 10 intensity Relative Film Optical Density Film Optical Underexposed 0 1 0.01 0.1 1 10 100 Exposure, mR 20000 2000 200 20 2 Sensitivity (S) Analog versus digital detectors • Analog -
Digital Imaging Ethics
Digital Imaging Ethics It is strongly advised that EMS Users follow the MSA Policy on Digital Image Manipulation. "Ethical digital imaging requires that the original uncompressed image file be stored on archival media (e.g., CD-R) without any image manipulation or processing operation. All parameters of the production and acquisition of this file, as well as any subsequent processing steps, must be documented and reported to ensure reproducibility. Generally, acceptable (non-reportable) imaging operations include gamma correction, histogram stretching, and brightness and contrast adjustments. All other operations (such as Unsharp-Masking, Gaussian Blur, etc.) must be directly identified by the author as part of the experimental methodology. However, for diffraction data or any other image data that is used for subsequent quantification, all imaging operations must be reported." This policy was formulated by the Digital Image Processing & Ethics Group of the MSA Education Committee and was adopted as MSA policy at the Summer Council meeting August 2-3, 2003. Guidelines for the proper acquisition and manipulation of scientific digital images: (from Douglas W. Cromey, M.S. - Manager, Cellular Imaging Core Southwest Environmental Health Sciences Center, University of Arizona, Tucson, Arizona) See here for the original article These guidelines were written for life science imaging but are relevant to materials science microscopy as well. 1. Scientific digital images are data that can be compromised by inappropriate manipulations. Images are data arranged spatially in an XY matrix (or grid) and each individual element (pixel) has a numerical value that represents a grayscale or RGB intensity value. These data are a numerical sampling of the specimen as presented by the data acquisition system (e.g., microscope) to the sensor (e.g., CCD camera). -
Digital Imaging and Printing Selection 92 Image Manipulation Requires Selecting Either a Part of the Image Or the Entire Image to Make Changes
90 CHAPTER DIGITAL IMAGING and 08 PRINTING Towards a New AgeDesign a New Graphic Towards raphic designers work with visual images, either for Gprint media or for digital media. With the advent of 91 computers, most of the graphic designer’s work is being done using computers. From graphical point of view there is a vast difference between images on paper such as drawings, sketches or photographs and images that you see on the screen of the computers. Images that are created, manipulated and displayed using computers are called digital images. Digital images are different from images drawn or painted on paper in many ways. TYPES OF DIGITAL IMAGES There are two major categories of digital images: raster images and vector images. When images are stored in a computer in the form of a grid of basic picture elements called pixels, then these images are called raster images. The pixels contain the information about colour and brightness. Image-editing programmes can replace or modify the pixels to edit the image Digital Imaging and Imaging Printing Digital in various ways. The pixels can be modified in groups, or individually. There are sophisticated algorithms to achieve this. On the other hand vector images are stored as mathematical descriptions of the image in terms of lines, Bezier curves, and text instead of pixels. This is the main difference between raster and vector images. However, this difference is responsible for the development of two major categories of graphic technologies namely: Raster Graphics and Vector Graphics. Therefore, the image-editing software used by the practicing graphic designers falls under one of these categories. -
Avalanche Photodiodes Arrays
Rochester Institute of Technology RIT Scholar Works Theses 2004 Avalanche photodiodes arrays Daniel Ma Follow this and additional works at: https://scholarworks.rit.edu/theses Recommended Citation Ma, Daniel, "Avalanche photodiodes arrays" (2004). Thesis. Rochester Institute of Technology. Accessed from This Thesis is brought to you for free and open access by RIT Scholar Works. It has been accepted for inclusion in Theses by an authorized administrator of RIT Scholar Works. For more information, please contact [email protected]. Avalanche Photodiodes Arrays By Daniel Ma B.S. College of Engineering, Rochester Institute of Technology (1998) A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in the Chester F. Carlson Center for Imaging Science of the College of Science Rochester Institute of Technology August 2004 Signature of the Author __D_a_n_i e_1 _M_a_______ _ Accepted by Harvey E. Rhody .y/h~~s- ) Coordinator, M.S. Degree Program Date CHESTERF.CARLSON CENTER FOR IMAGING SCIENCE COLLEGE OF SCIENCE ROCHESTER INSTITUTE OF TECHNOLOGY ROCHESTER, NEW YORK CERTIFICATE OF APPROVAL M.S. DEGREE THESIS The M.S. Degree Thesis of Daniel Ma has been examined and approved by the thesis committee as satisfactory for the thesis requirement for the Master of Science degree Zoran Ninkov Dr. Zoran Ninkov, Thesis Advisor Lynn Fuller Dr. Lynn Fuller Jonathan S. Arney Dr. Jon Arney Date ii THESIS RELEASE PERMISSION ROCHESTER INSTITUTE OF TECHNOLOGY COLLEGE OF SCIENCE CHESTER F. CARLSON CENTER FOR IMAGING SCIENCE Title of Thesis: Avalanche Photodiode Arrays I, Daniel Ma, hereby grant permission to the Wallace Memorial Library of R.I.T.