Chapter 4: High Energy X-Ray Generators: Linear Accelerators
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Design and Testing of Collimators for Use in Measuring X-Ray Attenuation
DESIGN AND TESTING OF COLLIMATORS FOR USE IN MEASURING X-RAY ATTENUATION By RAJESH PANTHI Master of Science (M.Sc.) in Physics Tribhuvan University Kathmandu, Nepal 2009 Submitted to the Faculty of the Graduate College of the Oklahoma State University in partial fulfillment of the requirements for the Degree of MASTER OF SCIENCE December, 2017 DESIGN AND TESTING OF COLLIMATORS FOR USE IN MEASURING X-RAY ATTENUATION Thesis Approved: Dr. Eric R. Benton Thesis Adviser and Chair Dr. Eduardo G. Yukihara Dr. Mario F. Borunda ii ACKNOWLEDGEMENTS I would like to express the deepest appreciation to my thesis adviser As- sociate Professor Dr. Eric Benton of the Department of Physics at Oklahoma State University for his vigorous guidance and help in the completion of this work. He provided me all the academic resources, an excellent lab environment, financial as- sistantship, and all the lab equipment and materials that I needed for this project. I am grateful for many skills and knowledge that I gained from his classes and personal discussion with him. I would like to thank Adjunct Profesor Dr. Art Lucas of the Department of Physics at Oklahoma State University for guiding me with his wonderful experience on the Radiation Physics. My sincere thank goes to the members of my thesis committee: Professor Dr. Eduardo G. Yukihara and Assistant Professor Dr. Mario Borunda of the Department of Physics at Oklahoma State University for generously offering their valuable time and support throughout the preparation and review of this document. I would like to thank my colleague Mr. Jonathan Monson for helping me to access the Linear Accelerators (Linacs) in St. -
Cathode-Ray Tube Displays for Medical Imaging
DIGITAL IMAGING BASICS Cathode-Ray Tube Displays for Medical Imaging Peter A. Keller This paper will discuss the principles of cathode-ray crease the velocity of the electron beam for tube displays in medical imaging and the parameters increased light output from the screen; essential to the selection of displays for specific 4. a focusing section to bring the electron requirements. A discussion of cathode-ray tube fun- beam to a sharp focus at the screen; damentals and medical requirements is included. 9 1990bu W.B. Saunders Company. 5. a deflection system to position the electron beam to a desired location on the screen or KEY WORDS: displays, cathode ray tube, medical scan the beam in a repetitive pattern; and irnaging, high resolution. 6. a phosphor screen to convert the invisible electron beam to visible light. he cathode-ray tube (CRT) is the heart of The assembly of electrodes or elements mounted T almost every medical display and its single within the neck of the CRT is commonly known most costly component. Brightness, resolution, as the "electron gun" (Fig 2). This is a good color, contrast, life, cost, and viewer comfort are analogy, because it is the function of the electron gun to "shoot" a beam of electrons toward the all strongly influenced by the selection of a screen or target. The velocity of the electron particular CRT by the display designer. These beam is a function of the overall accelerating factors are especially important for displays used voltage applied to the tube. For a CRT operating for medical diagnosis in which patient safety and at an accelerating voltage of 20,000 V, the comfort hinge on the ability of the display to electron velocity at the screen is about present easily readable, high-resolution images 250,000,000 mph, or about 37% of the velocity of accurately and rapidly. -
Review of Power Sources
RF Power Generation With Klystrons amongst other things Dr. C Lingwood Includes slides by Professor R.G. Carter and A Dexter Engineering Department, Lancaster University, U.K. and The Cockcroft Institute of Accelerator Science and Technology • Basic Klystron Principals • Existing technology • Underrating • Modulation anodes • Other options – IOTS – Magnetrons June 2011 ESS Workshop June 2 IOT June 2011 ESS Workshop June 3 IOT Output gap June 2011 ESS Workshop June 4 Velocity modulation • An un-modulated electron beam passes through a cavity resonator with RF input • Electrons accelerated or retarded according to the phase of the gap voltage: Beam is velocity modulated: • As the beam drifts downstream bunches of electrons are formed as shown in the Applegate diagram • An output cavity placed downstream extracts RF power just as in an IOT • This is a simple 2-cavity klystron • Conduction angle = 180° (Class B) June 2010 CAS RF for Accelerators, Ebeltoft 5 Multi-cavity klystron • Additional cavities are used to increase gain, efficiency and bandwith • Bunches are formed by the first (N-1) cavities • Power is extracted by the Nth cavity • Electron gun is a space- charge limited diode with perveance given by I0 K 3 2 V0 • K × 106 is typically 0.5 - 2.0 • Beam is confined by an axial magnetic field Photo courtesy of Thales Electron Devices June 2010 CAS RF for Accelerators, Ebeltoft 6 Efficiency and Perveance • Second harmonic cavity used to increase bunching • Maximum possible efficiency with second harmonic cavity is approximately 6 e 0.85 -
ADVANCED SPECTROMETER Introduction
ADVANCED SPECTROMETER Introduction In principle, a spectrometer is the simplest of scientific very sensitive detection and precise measurement, a real instruments. Bend a beam of light with a prism or diffraction spectrometer is a bit more complicated. As shown in Figure grating. If the beam is composed of more than one color of 1, a spectrometer consists of three basic components; a light, a spectrum is formed, since the various colors are collimator, a diffracting element, and a telescope. refracted or diffracted to different angles. Carefully measure The light to be analyzed enters the collimator through a the angle to which each color of light is bent. The result is a narrow slit positioned at the focal point of the collimator spectral "fingerprint," which carries a wealth of information lens. The light leaving the collimator is therefore a thin, about the substance from which the light emanates. parallel beam, which ensures that all the light from the slit In most cases, substances must be hot if they are to emit strikes the diffracting element at the same angle of inci- light. But a spectrometer can also be used to investigate cold dence. This is necessary if a sharp image is to be formed. substances. Pass white light, which contains all the colors of The diffracting element bends the beam of light. If the beam the visible spectrum, through a cool gas. The result is an is composed of many different colors, each color is dif- absorption spectrum. All the colors of the visible spectrum fracted to a different angle. are seen, except for certain colors that are absorbed by the gas. -
Comparative Overview of Inductive Output Tubes
! ESS AD Technical Note ! ESS/AD/0033 ! ! ! ! ! ! !!!!!!!!!! ! !!!Accelerator Division ! ! ! ! ! ! ! ! ! ! Comparative Overview of Inductive Output Tubes Rihua Zeng, Anders J. Johansson, Karin Rathsman and Stephen Molloy Influence of the Droop and Ripple of Modulator onRebecca Klystron SeviourOutput June 2011 23 February 2012 I. Introduction An IOT is a beam driven vacuum electronic RF amplifier. This document represents a comparative overview of the Inductive Output Tube (IOT). Starting with an overview of the IOT, we progress to a comparative discussion of the IOT relative to other RF amplifiers, discussing the advantages and limitations within the frame work of the RF amplifier requirements for the ESS. A discussion on the current state of the art in IOTs is presented along with the status of research programmes to develop 352MHz and 704MHz IOT’s. II. Background The Inductive Output Tube (IOT) RF amplifier was first proposed by Haeff in 1938, but not really developed into a working technology until the 1980s. Although primarily developed for the television transmitters, IOTs have been, and currently are, used on a number of international high- powered particle accelerators, such as; Diamond, LANSCE, and CERN. This has created a precedence and expertise in their use for accelerator applications. IOTs are a modified form of conventional coaxial gridded tubes, similar to the tetrode, although modified towards a linear beam structure device, similar to a Klystron. This hybrid construct is sometimes described as a cross between a klystron and a triode, hence Eimacs trade name for IOTs, the Klystrode. A schematic of an IOT, taken from [1], is shown in Figure 1. -
Solid State Modulators – Efficiency Considerations Focussing on Sic Devices –
Eidgenössische Technische Hochschule Zürich Laboratory for High Swiss Federal Institute of Technology Zurich Power Electronic Systems Solid State Modulators – Efficiency Considerations focussing on SiC Devices – J. Biela, S. Stathis, M. Jaritz, and S. Blume www.hpe.ee.ethz.ch / [email protected] Typical Topology of Solid State Pulse Modulator Systems AC/DC rectifier unit DC/DC converter for charging C-bank / voltage adaption Pulse generation unit Load e.g. klystron Constant Power Pulsed Power AC DC Energy Storage Pulse Klystron Modulator Load DC DC Grid Medium Voltage ⎧⎪⎪⎪⎨⎪⎪⎪⎩ Sometimes integrated V V V V t Pulse t t t Pulse 400V or MV Intermediate Buffer Capacitor Bank Pulse Voltage High Power 2 33 Electronic Systems Typical Topology of Solid State Pulse Modulator Systems Grounded klystron load I Isolation with 50Hz transformer or I Isolated DC-DC converter Typical Isolation AC DC Energy Storage Pulse Klystron Modulator Load DC DC Grid Medium Voltage V V V V t Pulse t t t Pulse 400V or MV Intermediate Buffer Capacitor Bank Pulse Voltage High Power 3 33 Electronic Systems 29 MW(35MW)/140 µs Modulator for CLIC – System Efficiency – High Power Electronic Systems CLIC System Specifications Output voltage 150:::180 kV Settling time <8 µs Output power (pulsed) 29 MW (- 35 MW) Repetition rate 50 Hz Flat-top length 140 µs Average output power 203 kW (- 245 kW) Flat-top stability (FTS) <0.85 % Pulse to pulse repeatab. <100 ppm Rise time <3 µs 819 klystrons 819 klystrons 15 MW, 142 µs circumferences 15 MW, 142 µs delay loop 73 m drive beam -
Gan Or Gaas, TWT Or Klystron - Testing High Power Amplifiers for RADAR Signals Using Peak Power Meters
Application Note GaN or GaAs, TWT or Klystron - Testing High Power Amplifiers for RADAR Signals using Peak Power Meters Vitali Penso Applications Engineer, Boonton Electronics Abstract Measuring and characterizing pulsed RF signals used in radar applications present unique challenges. Unlike communication signals, pulsed radar signals are “on” for a short time followed by a long “off” period, during “on” time the system transmits anywhere from kilowatts to megawatts of power. The high power pulsing can stress the power amplifier (PA) in a number of ways both during the on/off transitions and during prolonged “on” periods. As new PA device technologies are introduced, latest one being GaN, the behavior of the amplifier needs to be thoroughly tested and evaluated. Given the time domain nature of the pulsed RF signal, the best way to observe the performance of the amplifier is through time domain signal analysis. This article explains why the peak power meter is a must have test instrument for characterizing the behavior of pulsed RF power amplifiers (PA) used in radar systems. Radar Power Amplifier Technology Overview Peak Power Meter for Pulsed RADAR Measurements Before we look at the peak power meter and its capabilities, let’s The most critical analysis of the pulsed RF signal takes place in the look at different technologies used in high power amplifiers (HPA) time domain. Since peak power meters measure, analyze and dis- for RADAR systems, particularly GaN on SiC, and why it has grabbed play the power envelope of a RF signal in the time domain, they the attention over the past decade. -
Design and Emission Uniformity Studies of a 1.5-MW Gyrotron Electron Gun
PSFC/JA-03-1 Design and Emission Uniformity Studies of a 1.5-MW Gyrotron Electron Gun Anderson, J. P., Korbly, S. E., Temkin, R. J., Shapiro, M. A., Felch, K. L.*, Cauffman, S.* December 2002 Plasma Science and Fusion Center Massachusetts Institute of Technology Cambridge, MA 02139 USA * Microwave Power Products Division Communications and Power Industries Palo Alto, CA 94303 USA This work was supported by the U.S. Department of Energy, Office of Fusion Sciences and Virtual Laboratory for Technology. Reproduction, translation, publication, use and disposal, in whole or in part, by or for the United States government is permitted. Submitted for publication to IEEE Transactions on Plasma Science. 1 Design and Emission Uniformity Studies of a 1.5 MW Gyrotron Electron Gun James P. Anderson1, Stephen E. Korbly1, Richard J. Temkin1, Michael A. Shapiro1, K. L. Felch2, and S. Cauffman2 1Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, MA 02139 2Microwave Power Products Division, Communications and Power Industries, Palo Alto, CA 94303 Abstract We present the design and initial operation of a 96 kV, 40 A Magnetron Injection Gun (MIG) for a 1.5 MW, 110 GHz gyrotron. A critical parameter for the successful application of this electron gun is the uniformity of electron emission. The I-V curve of emission, at a series of temperatures, is measured. Analysis indicates that the work function of the emitter is 1.6 eV with a (total) spread of 0.07 +/- 0.01 eV. Measurement of the azimuthal emission uniformity with a rotating probe indicates that the work function variation around the azimuth, the global spread, is 0.04+/- 0.02 eV. -
Arecibo 430 Mhz Radar System
file: 430txman 12-98 draft Aug. 31, 2005 Arecibo 430 MHz Radar System Operation and Maintenance Manual Written by Jon Hagen April 2001, 2nd ed. May 2005 1 NOTE With its high-voltage and high-power, and high places, this transmitter is potentially lethal. Proper precautions must be taken to avoid electrical shock, RF exposure, and X-ray exposure. (See Section 22). Emergency Procedure: ELECTRIC SHOCK Neutralize power 1. De-energize the circuit by means of switch or circuit breaker or cut the line by an insulated cutter. 2. Safely remove the victim from contact with the energy source by using dry wood stick, plastic rope, leather belt, blanket or any other non-conductive materials. Call for help 1. Others can help you administer first aid 2. Others can call professional medical help and/or arrange transfer facilities Cardio Pulmonary Resuscitation (CPR) 1. Check victim's ABC A - airway: Clear and open airway by head tilt - chin lift maneuver B - breathing: Check and restore breathing by rescue breathing C- circulation: Check and restore circulation by external chest compression 2. If pulse is present, but not breathing, maintain one rescue breathing (mouth to mouth resuscitation) as long as necessary. 3. If pulse and breathing are absent, give external chest compressions (CPR). 4. If pulse and breathing are present, stop CPR, stabilize the victim. 5. Caution: Only properly trained personnel should administer CPR to avoid further harm to 2 the victim. Administer first aid for shock 1. Keep the victim lying down, warm and comfortable to maintain body heat until medical assistance arrive. -
Lhc Collimator Alignment Operational Tool∗
TUPPC120 Proceedings of ICALEPCS2013, San Francisco, CA, USA LHC COLLIMATOR ALIGNMENT OPERATIONAL TOOL∗ G. Valentinoy , CERN, Geneva, Switzerland and University of Malta, Msida, Malta R. W. Aßmannz , S. Redaelli, CERN, Geneva, Switzerland N. Sammut, University of Malta, Msida, Malta Abstract tor tanks housing the jaws and other equipment such as Beam-based LHC collimator alignment is necessary to quadrupole magnets and Beam Position Monitors (BPMs). determine the beam centers and beam sizes at the colli- The actual beam orbit may deviate from the design orbit mator locations for various machine configurations. Fast over several months of operation due to ground motion and and automatic alignment is provided through an opera- thermal effects [4]. Hence, all collimators are periodically tional tool has been developed for use in the CERN Con- aligned to the beam to determine these parameters. A jaw trol Center, which is described in this paper. The tool is is aligned when a sharp increase followed by a slow expo- implemented as a Java application, and acquires beam loss nential decrease appears in the signal read out from a Beam and collimator position data from the hardware through a Loss Monitoring (BLM) detector [5] placed downstream of middleware layer. The user interface is designed to allow the collimator. for a quick transition from application start up, to select- ing the required collimators for alignment and configuring OPERATIONAL TOOL the alignment parameters. The measured beam centers and Main Display sizes are then logged and displayed in different forms to A screenshot of the main display of the collimator appli- help the user set up the system. -
Evaluation of Infrared Collimators for Testing Thermal Imaging Systems
OPTO-ELECTRONICS REVIEW 15(2), 82–87 DOI: 10.2478/s11772-007-0005-9 Evaluation of infrared collimators for testing thermal imaging systems K. CHRZANOWSKI*1,2 1Institute of Optoelectronics, Military University of Technology, 2 Kaliskiego Str., 00-908 Warsaw, Poland 2INFRAMET, 24 Graniczna Str., Kwirynów, 05-082 Stare Babice, Poland Infrared reflective collimators are important components of expensive sophisticated test systems used for testing thermal imagers. Too low quality collimators can become a source of significant measurement errors and collimators of too high quality can unnecessarily increase cost of a test system. In such a situation it is important for test system users to know proper requirements on the collimator and to be able to verify its performance. A method for evaluation of infrared reflective collimators used in test systems for testing thermal imagers is presented in this paper. The method requires only easily avail- able optical equipment and can be used not only by collimator manufactures but also by users of test equipment to verify per- formance of the collimators used for testing thermal imagers. Keywords: IR systems, testing thermal imaging systems, IR optical design. 1. Introduction requirement that the collimator spatial resolution should match the spatial resolution capabilities of the tested thermal IR collimators are typical elements of laboratory sets-up used imager. for testing thermal imaging systems. Reflective two-mirror Although IR collimators are frequently used for testing collimators built using an off-axis parabolic collimating mir- thermal imagers since the 1970s, there has been little interest ror and smaller directional flat mirror represent a typical de- in a problem of evaluation of these optical systems. -
Low Emittance Thermionic Electron Gun at Slri
9th International Particle Accelerator Conference IPAC2018, Vancouver, BC, Canada JACoW Publishing ISBN: 978-3-95450-184-7 doi:10.18429/JACoW-IPAC2018-THPMK088 LOW EMITTANCE THERMIONIC ELECTRON GUN AT SLRI ∗ K. Kittimanapun , N. Juntong, C. Dhammatong, W. Phacheerak, and M. Phanak Synchrotron Light Research Institute (SLRI), Nakhon Ratchasima, Thailand Abstract • Fast beam deflector allowing nanosecond-pulsed elec- The Synchrotron Light Research Institute (SLRI) has de- tron beam to transport to the bunching section and to veloped a new thermionic electron gun producing low emit- deflect undesired electrons to the collimator. tance electron beam for the future upgrade of the existing • Pre-buncher and buncher to adiabatically bunch and one. The thermionic cathode made of a CeB single crys- 6 accelerate electrons to higher energy and minimize tal is selected due to its properties providing high electron the effect from the Radio-Frequency (RF) field that beam current, uniform current density, and high resistance potentially causes the emittance growth. to contamination. In addition, the CeB6 cathode of 3 mm in diameter can produce up to a few Amperes of electron beam ELECTRON GUN current. The electron gun is pulsed at 500 kV with a few microseconds wide to avoid high voltage breakdown as well Three main parts that have to be carefully considered for as to reduce space charge effect resulting in the emittance building the high-performance thermionic electron guns are growth of the extracted electron beam. The preliminary sim- an electron gun cathode, extraction of high-current electron ulation and design of the electron gun together with the high beam, and a high-voltage system.