A CdTe detector with a Gd converter for thermal neutron detection
|
|
- David George
- 5 years ago
- Views:
Transcription
1 A CdTe detector with a Gd converter for thermal neutron detection Aki Miyake, Takahiro Nishika, Shailendra Singh, Hisashi Morii, Hidenori Minura, Toru Aoki. Nuclear Instruments and Methods in Physics Research A 654 (2011) Paper review 12/12/11 Edward Cazalas
2 Objectives of Paper Create thermal neutron detector for neutron imaging with... High resolution Fast response time Room temperature operation. Thermal neutron detection through measurement of gamma energy in (n,g) reaction. Previous work done by group includes use of CdTe semiconductor for neutron detection Semiconductors have fast response times and operate at room temperature. Higher energy resolution is one purpose of this work
3 Objectives of Paper Modify use of CdTe semiconductor for neutron detection. Want high energy resolution to determine gammas generated in detector vs. those created in-beam (background) Obtain high energy resolution through application of higher electric fields in semiconductor make CdTe thinner. Use Gadolinium converter on top of CdTe to increase neutron attenuation lost by thinner CdTe.
4 Why Cadmium, Gadolinium. Thermal neutron (n,g) reaction Cadmium: ~12% 113 Cd (σ = 2.06E4 b) Tellurium: ~0.9% 123Te (σ = 370 b) Gadolinium: ~15% 155Gd (σ = 6.1E4 b), ~16% 155Gd (σ = 2.55E5 b) On average natural Gd has cross section 20 times higher than Cd How thick should Gd converter layer be? Use GEANT4
5 Detector construction CdTe is 4 x 4 x 0.5 mm Gd converter is 4 x 4 x? mm Gd converter is pasted with silver onto gold electrode Operation at 200V (why? Presume this voltage of max linear e- collection) Preamplifier (shaping time set at 0.5 us) Pulse height analyzer Assume indium electrode is negatively biased relative to the gold electrode. What about charge created in Gd converter?
6 Simulation of Gd Converter GEANT4 used to optimize Gd converter thickness to allow maximum photon collection by CdTe Assumed thermal neutron at ev Random distribution (xy position) beam source simulated neutrons Max at 25 um thick Gd
7 Potential issues with Simulation of Cd Converter Why simulated neutrons? Typically we only care about statistics. Plot should be gamma ray per neutron Error bars on plot... These are statistical means and need standard errors. Gd thickness... What about CdTe thickness? Are we stuck with a single thickness for a reason?
8 Simulation of Resolution Determine spatial resolution Infinitely narrow beam source centered in the middle of Gd converted Divide accumulated counts into 50 x 50 um pixels. Commercial CdTe pixel size = 100 x 100 um. Results give spread of 50 um one pixel Point spread function for 25 um Gd converter thickness
9 Simulation of Resolution Results give spread of 50 um one pixel FWHM of point spread function
10 Issues with Simulation of Resolution This plot does not portray very much information. Perhaps plot several peaks corresponding to several Gd converter thicknesses. Again, statistics What was the thickness of Gd converter? Not obvious.
11 Issues with Simulation of Resolution Why 50 x 50 um pixel size? What about smaller thickness Gd converters? Even a single data point below the selection point would be very useful in characterizing resolution behavior vs. Gd thickness
12 Build detector Irradiate Gd converter thickness = 25 um 241 Am = 59.5 kev gamma 57 Co = kev gamma 59.5 kev = 3.4 kev kev = 3.7 kev
13 Build detector Irradiate 252 Cf source (1.74 Mbq) surrounded by polyethylene moderator to thermalize emitted neutrons. Also surrounded by Lead and Tin to attenuate gammas (n,g) reaction prompt gammas = 157 Gd 80, 182 kev 155 Gd 199 kev 113 Cd 95 kev X-rays from Gd conversion electrons
14 Build detector Irradiate Spectrum background contains Compton events and background gammas from (n,g) reaction with lead, tin, polyethylene. It is claimed that neutron events are separable from background gammas. Technically true, however by the nature of the experiment, background gammas would not be expected to be strong.
15 Thoughts Would be nice to have quick calculation cross checking the simulated results to the experiment (could calculate total number of counts of all Gd(n,g) and Cd(n,g) gammas in spectrum and compare to estimated number of incident gammas in simulation). Would be interesting to see effectiveness of different design (wider CdTe, or Gd converter with CdTe on both sides, for example. Would likely shift optimum Gd converter to much larger thickness thereby increasing attenuation of neutrons without serious spacial losses of gammas). Simple to do in simulation. A simulation studying the response as a function of CdTe thickness (correlated with Gd converter thickness) would be valuable.
PERFORMANCE IMPROVEMENT OF CZT DETECTORS BY LINE ELECTRODE GEOMETRY
Applications of Nuclear Techniques (CRETE3) International Journal of Modern Physics: Conference Series Vol. 27 (24) 4644 (8 pages) The Authors DOI:.42/S294546446 PERFORMANCE IMPROVEMENT OF CZT DETECTORS
More informationEfficiency and Attenuation in CdTe Detectors
Efficiency and Attenuation in CdTe Detectors Amptek Inc. Bob Redus, May 5, 00 Amptek s XR-00T-CdTe is a high performance x-ray and gamma ray detector system. Like Amptek s other XR00 products, a detector
More informationPOSITION SENSITIVE DETECTION OF CONCEALED SUBSTANCES EMPLOYING PULSED SLOW NEUTRONS
POSITION SENSITIVE DETECTION OF CONCEALED SUBSTANCES EMPLOYING PULSED SLOW NEUTRONS R. E. Mayer A. Tartaglione, J. J. Blostein, M. Schneebeli, P. D Avanzo, L. Capararo Centro Atómico Bariloche and Instituto
More informationIntroduction to Radiological Sciences Neutron Detectors. Theory of operation. Types of detectors Source calibration Survey for Dose
Introduction to Radiological Sciences Neutron Detectors Neutron counting Theory of operation Slow neutrons Fast neutrons Types of detectors Source calibration Survey for Dose 2 Neutrons, what are they?
More informationDevelopment of Gamma-ray Monitor using CdZnTe Semiconductor Detector
Development of Gamma-ray Monitor using CdZnTe Semiconductor Detector A. H. D. Rasolonjatovo 1, T. Shiomi 1, T. Nakamura 1 Y. Tsudaka 2, H. Fujiwara 2, H. Araki 2, K. Matsuo 2, H. Nishizawa 2 1 Cyclotron
More informationDevelopment of High-Z Semiconductor Detectors and Their Applications to X-ray/gamma-ray Astronomy
Development of High-Z Semiconductor Detectors and Their Applications to X-ray/gamma-ray Astronomy Taka Tanaka (SLAC/KIPAC) 9/19/2007 SLAC Advanced Instrumentation Seminar Outline Introduction CdTe Diode
More informationNew trends in CdTe detectors for X and γ-ray applications
New trends in CdTe detectors for X and γ-ray applications Olivier Limousin CEA Saclay / DSM / DAPNIA Service d Astrophysique France New developments in photodetection, Beaune 2002 / Solid state detectors
More informationChemical Engineering 412
Chemical Engineering 412 Introductory Nuclear Engineering Lecture 26 Radiation Detection & Measurement II Spiritual Thought 2 I would not hold the position in the Church I hold today had I not followed
More informationInternational Journal of Scientific & Engineering Research, Volume 5, Issue 3, March-2014 ISSN
308 Angular dependence of 662 kev multiple backscattered gamma photons in Aluminium Ravindraswami K a, Kiran K U b, Eshwarappa K M b and Somashekarappa H M c* a St Aloysius College (Autonomous), Mangalore
More informationAlpha-particle Stopping Powers in Air and Argon
Alpha-particle Stopping Powers in Air and Argon Mohammad QH 1* and Maghdid HA 2 1 Department of Physics, College of Science, Raparin University, Sulaimanyah, Iraqi Kurdistan, Iraq 2 Department of Physics,
More informationWaste Characterization
Radiation Monitoring Systems & Waste Characterization Lecture 4 - Neutron Detectors M.Taiuti MASTER UNIVERSITARIO DI II LIVELLO IN SCIENZE E TECNOLOGIE DEGLI IMPIANTI NUCLEARI Neutron Detectors What does
More informationV. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber
CYRIC Annual Report 2001 V. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber Kawata N. Baba M. Kato M.*, Miura T.**, and Yamadera A.***, Cyclotron and Radioisotope Center, Tohoku
More informationProblem P7. Stéphanie Ménard. Dosimetry Department Fontenay-aux FRANCE IRSN QUADOS IRSN
Problem P7 Stéphanie Ménard Dosimetry Department 92262 Fontenay-aux aux-roses FRANCE What are the applications of Gamma-Ray Spectrometry in Radiological Protection and in Safety? In the environment: after
More informationFinal report on DOE project number DE-FG07-99ID High Pressure Xenon Gamma-Ray Spectrometers for Field Use
Final report on DOE project number DE-FG07-99ID13772 High Pressure Xenon Gamma-Ray Spectrometers for Field Use Principle Investigator: Glenn K. Knoll Co-investigator: David K. Wehe, Zhong He, University
More informationAdvantages / Disadvantages of semiconductor detectors
Advantages / Disadvantages of semiconductor detectors Semiconductor detectors have a high density (compared to gas detector) large energy loss in a short distance diffusion effect is smaller than in gas
More informationDevelopment and characterization of 3D semiconductor X-rays detectors for medical imaging
Development and characterization of 3D semiconductor X-rays detectors for medical imaging Marie-Laure Avenel, Eric Gros d Aillon CEA-LETI, DETectors Laboratory marie-laure.avenel@cea.fr Outlines Problematic
More informationChapter 11: Neutrons detectors
Chapter 11: Neutrons detectors 1 Contents Principles of neutrons detection Slow neutron detection methods Fast neutron detection methods 2 Introduction Neutrons are uncharged particles cannot be directly
More informationEE 5344 Introduction to MEMS CHAPTER 5 Radiation Sensors
EE 5344 Introduction to MEMS CHAPTER 5 Radiation Sensors 5. Radiation Microsensors Radiation µ-sensors convert incident radiant signals into standard electrical out put signals. Radiant Signals Classification
More informationCompton Camera. Compton Camera
Diagnostic Imaging II Student Project Compton Camera Ting-Tung Chang Introduction The Compton camera operates by exploiting the Compton Effect. It uses the kinematics of Compton scattering to contract
More informationDetecting high energy photons. Interactions of photons with matter Properties of detectors (with examples)
Detecting high energy photons Interactions of photons with matter Properties of detectors (with examples) Interactions of high energy photons with matter Cross section/attenution length/optical depth Photoelectric
More informationTrace Element Analysis of Geological, Biological & Environmental Materials By Neutron Activation Analysis: An Exposure
Trace Element Analysis of Geological, Biological & Environmental Materials By Neutron Activation Analysis: An Exposure ILA PILLALAMARRI Earth Atmospheric & Planetary Sciences Neutron Activation Analysis
More informationSupplemental information for Positron-Induced Luminescence. Abstract
Supplemental information for Positron-Induced Luminescence E. V. Stenson, U. Hergenhahn, M. R. Stoneking, and T. Sunn Pedersen (Dated: April 6, 2018) Abstract This document provides supplemental information
More informationFast Neutron and Gamma-Ray Detectors for the CSIRO Air Cargo Scanner
Fast Neutron and Gamma-Ray Detectors for the CSIRO Air Cargo Scanner J.E. Eberhardt, A.J. McEwan, D. Milinkovic, V. Sharp, * and J.R. Tickner CSIRO Minerals, Private Mail Bag 5, Menai NSW 2234 Australia
More informationInternational Journal of Scientific & Engineering Research, Volume 5, Issue 3, March-2014 ISSN
316 Effective atomic number of composite materials by Compton scattering - nondestructive evaluation method Kiran K U a, Ravindraswami K b, Eshwarappa K M a and Somashekarappa H M c* a Government Science
More informationA new neutron monitor for pulsed fields at high-energy accelerators
A new neutron monitor for pulsed fields at high-energy accelerators Marlies Luszik-Bhadra *, Eike Hohmann Physikalisch-Technische Bundesanstalt, Bundesallee 100, D-38116, Braunschweig, Germany. Abstract.
More informationA Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS
A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS Name of contact person: Surender Kumar Sharma Name of other contributors: R.
More informationDevelopment of a new MeV gamma-ray camera
Development of a new MeV gamma-ray camera ICEPP Symposium February 16, 2004 Hakuba, Nagano, Japan Kyoto University Atsushi Takeda H. Kubo, K. Miuchi, T. Nagayoshi, Y. Okada, R. Orito, A. Takada, T. Tanimori,
More informationDetection of X-Rays. Solid state detectors Proportional counters Microcalorimeters Detector characteristics
Detection of X-Rays Solid state detectors Proportional counters Microcalorimeters Detector characteristics Solid State X-ray Detectors X-ray interacts in material to produce photoelectrons which are collected
More informationHe-3 Neutron Detectors
Application He-3 Neutron Detectors General Considerations, Applications: He-3 filled proportional counters are standard neutron detectors and are most suitable for the detection of thermal neutrons. Larger
More informationSemiconductor Thermal Neutron Detector
Semiconductor Thermal Neutron Detector Toru Aoki 1,3, Aki Miyake 2,3, Takayuki Nakano 2, Akifumi Koike 1,3, Hisashi Morii 2, and Hidenori Mimura 1 1. Research Institute of Electronics, Shizuoka University,
More informationRecent Activities on Neutron Calibration Fields at FRS of JAERI
Recent Activities on Neutron Calibration Fields at FRS of JAERI Michio Yoshizawa, Yoshihiko Tanimura, Jun Saegusa and Makoto Yoshida Department of Health Physics, Japan Atomic Energy Research Institute
More informationA Study On Radioactive Source Imaging By Using A Pixelated CdTe Radiation Detector
ISSN: 1791-4469 Copyright 2012 Hellenic Naval Academy A Study On Radioactive Source Imaging By Using A Pixelated CdTe Radiation Detector K. Zachariadou a,c, K. Karafasoulis b,c, S. Seferlis c, I. Papadakis
More informationApplied Nuclear Physics (Fall 2006) Lecture 21 (11/29/06) Detection of Nuclear Radiation: Pulse Height Spectra
22.101 Applied Nuclear Physics (Fall 2006) Lecture 21 (11/29/06) Detection of Nuclear Radiation: Pulse Height Spectra References: W. E. Meyerhof, Elements of Nuclear Physics (McGraw-Hill, New York, 1967),
More informationTIIVISTELMÄRAPORTTI (SUMMARY REPORT)
2014/2500-0002M ISSN 1797-3457 (verkkojulkaisu) ISBN (PDF) 978-951-25-2627-7 978-951- TIIVISTELMÄRAPORTTI (SUMMARY REPORT) Detection of CBRNE materials using active neutron interrogation (CBRNE-aineiden
More informationSlides by: Prof. Abeer Alharbi
Slides by: Prof. Abeer Alharbi electromagnetic radiation of high energy. They are produced by sub-atomic particle interactions, such as electron-positron annihilation, neutral pion decay, radioactive decay,
More informationThe interaction of radiation with matter
Basic Detection Techniques 2009-2010 http://www.astro.rug.nl/~peletier/detectiontechniques.html Detection of energetic particles and gamma rays The interaction of radiation with matter Peter Dendooven
More informationPerformance of high pressure Xe/TMA in GEMs for neutron and X-ray detection
Performance of high pressure Xe/TMA in GEMs for neutron and X-ray detection R. Kreuger, C. W. E. van Eijk, Member, IEEE, F. A. F. Fraga, M. M. Fraga, S. T. G. Fetal, R. W. Hollander, Member, IEEE, L. M.
More informationMeasurements of liquid xenon s response to low-energy particle interactions
Measurements of liquid xenon s response to low-energy particle interactions Payam Pakarha Supervised by: Prof. L. Baudis May 5, 2013 1 / 37 Outline introduction Direct Dark Matter searches XENON experiment
More informationNeutron activation analysis. Contents. Introduction
Neutron activation analysis Contents Neutron activation analysis... 1 Introduction... 1 Principle of method... 2 Detection of radionuclides... 3 Kinetics of activation... 4 Choosing the appropriate procedure...
More informationMeasurement of Average Thermal Neutron Flux for PGNAA Setup
2017 IJSRST Volume 3 Issue 8 Print ISSN: 2395-6011 Online ISSN: 2395-602X Themed Section: Science and Technology Measurement of Average Thermal Neutron Flux for PGNAA Setup Dalpat Meena 1, S. K. Gupta
More informationPHYS 3650L - Modern Physics Laboratory
PHYS 3650L - Modern Physics Laboratory Laboratory Advanced Sheet Photon Attenuation 1. Objectives. The objectives of this laboratory exercise are: a. To measure the mass attenuation coefficient at a gamma
More informationNuclear Lifetimes. = (Eq. 1) (Eq. 2)
Nuclear Lifetimes Theory The measurement of the lifetimes of excited nuclear states constitutes an important experimental technique in nuclear physics. The lifetime of a nuclear state is related to its
More informationDigital simulation of neutron and gamma measurement devices
3Security of radioactive materials and transport 3 2 Digital simulation of neutron and gamma measurement devices A.-L. WEBER (IRSN) 1 - Maximum activity that a radioactive element can present without being
More informationNext Generation Scintillation Detectors: Development of Quantum Dot Doped Scintillator. Lindley Winslow University of California Los Angeles
Next Generation Scintillation Detectors: Development of Quantum Dot Doped Scintillator Lindley Winslow University of California Los Angeles I am particularly interested in applications to... e - e - νi
More informationNew perspectives in X-ray detection of concealed illicit materials brought by CdTe/CdZnTe spectrometric detectors
New perspectives in X-ray detection of concealed illicit materials brought by CdTe/CdZnTe spectrometric detectors Jean-Marc Dinten, Jean-Louis Amans, Loïck Verger, Olivier Peyret CEA-LETI, MINATEC, Recherche
More informationINTERACTIONS OF RADIATION WITH MATTER
INTERACTIONS OF RADIATION WITH MATTER Renée Dickinson, MS, DABR Medical Physicist University of Washington Medical Center Department of Radiology Diagnostic Physics Section Outline Describe the various
More informationGamma and X-Ray Detection
Gamma and X-Ray Detection DETECTOR OVERVIEW The kinds of detectors commonly used can be categorized as: a. Gas-filled Detectors b. Scintillation Detectors c. Semiconductor Detectors The choice of a particular
More informationDetermination of the shielding power of different materials against gamma radiation
Determination of the shielding power of different materials against gamma radiation Chow Wing Yan, Yeung Chun Lap S.K.H Tsang Shiu Tim Secondary School Wong Ka Wing Baptist Lui Ming Choi Secondary School
More informationMeasurement of material uniformity using 3-D position sensitive CdZnTe gamma-ray spectrometers
Nuclear Instruments and Methods in Physics Research A 441 (2000) 459}467 Measurement of material uniformity using 3-D position sensitive CdZnTe gamma-ray spectrometers Z. He *, W.Li, G.F. Knoll, D.K. Wehe,
More informationAnalysis of γ spectrum
IFM The Department of Physics, Chemistry and Biology LAB 26 Analysis of γ spectrum NAME PERSONAL NUMBER DATE APPROVED I. OBJECTIVES - To understand features of gamma spectrum and recall basic knowledge
More informationQuality Assurance. Purity control. Polycrystalline Ingots
Quality Assurance Purity control Polycrystalline Ingots 1 Gamma Spectrometry Nuclide Identification Detection of Impurity Traces 1.1 Nuclides Notation: Atomic Mass Atomic Number Element Neutron Atomic
More informationBoron-based semiconductor solids as thermal neutron detectors
Boron-based semiconductor solids as thermal neutron detectors Douglas S. McGregor 1 and Stan M. Vernon 2 1 S.M.A.R.T. Laboratory, Department of Nuclear Engineering and Radiological Sciences, University
More informationGAMMA DETECTORS FOR High energy Inelastic Neutron Scattering. E.M. Schooneveld
GAMMA DETECTORS FOR High energy Inelastic Neutron Scattering E.M. Schooneveld Gamma detectors for HINS Collaboration: University of Rome Tor Vergata: - C. Andreani, S. Imberti, A. Pietropaolo, R. Senesi
More informationChem 481 Lecture Material 3/20/09
Chem 481 Lecture Material 3/20/09 Radiation Detection and Measurement Semiconductor Detectors The electrons in a sample of silicon are each bound to specific silicon atoms (occupy the valence band). If
More informationRadiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons
Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na Ellen Simmons 1 Contents Introduction Review of the Types of Radiation Charged Particle Radiation Detection Review of Semiconductor
More informationExam 4. P202 Spring 2004 Instructor: Prof. Sinova
Exam 4 P202 Spring 2004 Instructor: Prof. Sinova Name: Date: 4/22/04 Section: All work must be shown to get credit for the answer marked. You must show or state your reasoning. If the answer marked does
More informationEnergy calibration of the threshold of Medipix for ATLAS
Energy calibration of the threshold of Medipix for ATLAS Céline Lebel Université de Montréal lebel@lps.umontreal.ca presenting for the Institut of Experimental and Applied Physics of the Czech Technical
More informationChapter 4 Scintillation Detectors
Med Phys 4RA3, 4RB3/6R03 Radioisotopes and Radiation Methodology 4-1 4.1. Basic principle of the scintillator Chapter 4 Scintillation Detectors Scintillator Light sensor Ionizing radiation Light (visible,
More informationDEVELOPMENT OF NEUTRON INTERROGATION TECHNIQUES TO DETECT DANGEROUS SUBSTANCES
DEVELOPMENT OF NEUTRON INTERROGATION TECHNIQUES TO DETECT DANGEROUS SUBSTANCES Natalia M. B. D Amico, Ing. Roberto E. Mayer, Dr. Balseiro Institute, Bariloche Atomic Center, CNEA, Argentina National University
More informationDevelopment of New MicroStrip Gas Chambers for X-ray Applications
Joint International Workshop: Nuclear Technology and Society Needs for Next Generation Development of New MicroStrip Gas Chambers for X-ray Applications H.Niko and H.Takahashi Nuclear Engineering and Management,
More informationEffect of the time characteristics of the Compton camera on its performance
Effect of the time characteristics of the Compton camera on its performance Chibueze Zimuzo Uche Howell Round Michael Cree School of Engineering University of Waikato Introduction Anger camera Compton
More information(10%) (c) What other peaks can appear in the pulse-height spectrum if the detector were not small? Give a sketch and explain briefly.
Sample questions for Quiz 3, 22.101 (Fall 2006) Following questions were taken from quizzes given in previous years by S. Yip. They are meant to give you an idea of the kind of questions (what was expected
More informationarxiv: v1 [physics.ins-det] 29 Jun 2011
Investigation of Large LGB Detectors for Antineutrino Detection P. Nelson a,, N. S. Bowden b, a Department of Physics, Naval Postgraduate School, Monterey, CA 99, USA b Lawrence Livermore National Laboratory,
More informationPOSITIONING OF STEEL RODS INCLUSIONS IN REINFORCED CONCRETE SIMULANT BY COMPTON BACKSCATTERING
2011 International Nuclear Atlantic Conference - INAC 2011 Belo Horizonte,MG, Brazil, October 24-28, 2011 ASSOCIAÇÃO BRASILEIRA DE ENERGIA NUCLEAR - ABEN ISBN: 978-85-99141-04-5 POSITIONING OF STEEL RODS
More informationDEVELOPMENT OF ADVANCED NEUTRON INDUCED PROMPT GAMMA- RAY ANALYSIS SYSTEM FOR SURVEY OF ANTI-PERSONNEL MINES
DEVELOPMENT OF ADVANCED NEUTRON INDUCED PROMPT GAMMA- RAY ANALYSIS SYSTEM FOR SURVEY OF ANTI-PERSONNEL MINES T. Iguchi 1, J. Kawarabayashi 1, K. Watanabe 1, K. Nishimura 2, T. Handa 2 and H. Sawamura 2
More informationSilicon Drift Detectors for gamma-ray detection: 15 years of research (and collaboration between Politecnico and INAF-Milano)
Silicon Drift Detectors for gamma-ray detection: 15 years of research (and collaboration between Politecnico and INAF-Milano) Outline The Silicon Drift Detector (SDD) Gamma-ray detectors based on scintillators
More informationGamma and X-Ray Standards
Gamma and X-Ray Standards A wide range of gamma and x-ray standards for research and educational use are available in the energy range of 5.9 to 2614 kev. Many nuclides are available up to 100 µci (3.7
More informationScience of Nuclear Energy and Radiation a Comprehensive Course for Science Teachers June 22-25, 1998 McMaster University
Science of Nuclear Energy and Radiation a Comprehensive Course for Science Teachers June 22-25, 1998 McMaster University Notes to accompany Lab demonstrations by Barry Diacon, Technician, Department of
More informationMeasurement of the n_tof beam profile in the second experimental area (EAR2) using a silicon detector
Measurement of the n_tof beam profile in the second experimental area (EAR) using a silicon detector Fidan Suljik Supervisors: Dr. Massimo Barbagallo & Dr. Federica Mingrone September 8, 7 Abstract A new
More informationMONTE-CARLO SIMULATIONS OF TIME- RESOLVED, OPTICAL READOUT DETECTOR for PULSED, FAST-NEUTRON TRANSMISSION SPECTROSCOPY (PFNTS)
MONTE-CARLO SIMULATIONS OF TIME- RESOLVED, OPTICAL READOUT DETECTOR for PULSED, FAST-NEUTRON TRANSMISSION SCTROSCOPY (PFNTS) a*, David Vartsky a, I. Mardor a, M. B. Goldberg a, D. Bar a, G. Feldman a,
More informationQUIZ: Physics of Nuclear Medicine Atomic Structure, Radioactive Decay, Interaction of Ionizing Radiation with Matter
QUIZ: Physics of Nuclear Medicine Atomic Structure, Radioactive Decay, Interaction of Ionizing Radiation with Matter 1. An atomic nucleus contains 39 protons and 50 neutrons. Its mass number (A) is a)
More informationGeant4 Monte Carlo code application in photon interaction parameter of composite materials and comparison with XCOM and experimental data
Indian Journal of Pure & Applied Physics Vol. 54, Februray 2016, pp. 137-143 Geant4 Monte Carlo code application in photon interaction parameter of composite materials and comparison with XCOM and experimental
More informationX- & γ-ray Instrumentation
X- & γ-ray Instrumentation Used nuclear physics detectors Proportional Counters Scintillators The Dark Ages Simple collimators HEAO A1 & A2: 2 x 8 degree field of view Confusion limit is about 200 sources
More informationRESULTS AND DISCUSSION ON EFFECT OF COLLIMATOR SIZE ON THE ATTENUATION OF GAMMA RAY IN PURE ELEMENTS
CHAPTER RESULTS AND DISCUSSION ON EFFECT OF COLLIMATOR SIZE ON THE ATTENUATION OF GAMMA RAY IN PURE ELEMENTS 5.1 INTRODUCTION The increasing use of isotopes in the field of medicine and biology has demands
More informationHigh-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy
High-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy Thomas Niedermayr, I. D. Hau, S. Terracol, T. Miyazaki, S. E. Labov and S. Friedrich Former colleagues: M. F. Cunningham, J. N.
More informationTHE spectroscopic performance of large volume CdZnTe
3098 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 51, NO. 6, DECEMBER 2004 Analysis of Detector Response Using 3-D Position-Sensitive CZT Gamma-Ray Spectrometers Feng Zhang, Student Member, IEEE, Zhong He,
More informationPhotofission of 238-U Nuclei
Photofission of 238-U Nuclei International Thorium Energy Conference - ThEC18, 29-31st of October 2018, Belgium İsmail Boztosun This research has been supported by TÜBİTAK with grant number 114F220 Motivations
More informationPhysics 102: Lecture 26. X-rays. Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1
Physics 102: Lecture 26 X-rays Make sure your grade book entries are correct. Physics 102: Lecture 26, Slide 1 But first a quick review of the periodic table http://www.youtube.com/watch?v=smwlzwgmmwc
More informationSENSITIVITY ANALYSIS TO EVALUATE THE TRANSPORT PROPERTIES OF CdZnTe DETECTORS USING ALPHA PARTICLES AND LOW-ENERGY GAMMA-RAYS
http://dx.doi.org/10.5516/net.2011.43.6.567 SENSITIVITY ANALYSIS TO EVALUATE THE TRANSPORT PROPERTIES OF CdZnTe DETECTORS USING ALPHA PARTICLES AND LOW-ENERGY GAMMA-RAYS KYUNG-O KIM 1, WOO SANG AHN 2,
More informationThe Compton Effect. Martha Buckley MIT Department of Physics, Cambridge, MA (Dated: November 26, 2002)
The Compton Effect Martha Buckley MIT Department of Physics, Cambridge, MA 02139 marthab@mit.edu (Dated: November 26, 2002) We measured the angular dependence of the energies of 661.6 kev photons scattered
More informationCHAPTER 5 EFFECTIVE ATOMIC NUMBER OF SELECTED POLYMERS BY GAMMA BACKSCATTERING TECHNIQUE
CHAPTER 5 EFFECTIVE ATOMIC NUMBER OF SELECTED POLYMERS BY GAMMA BACKSCATTERING TECHNIQUE Page no. 5.1 Introduction 132 5.2 Methods and measurements 132 5.3 Saturation thickness of elements and polymers
More informationChapter Seven (Nuclear Detectors)
Al-Mustansiriyah University College of Science Physics Department Fourth Grade Nuclear Physics Dr. Ali A. Ridha Chapter Seven (Nuclear Detectors) Ionizing radiation is rarely detected directly. Instead,
More informationIn order to get the energy response of the CZT detector, the measurements were done using the mono-energetic X-ray beam sources from 10 to 40 kev and
Proceedings of the Second International Workshop on EGS, 8.-12. August 2000, Tsukuba, Japan KEK Proceedings 200-20, pp.144-151 Development of Gamma Ray Monitor Using CdZnTe Semiconductor Detector A. H.
More informationCdZnTe for Simultaneous Detection. 241-Am source. X-rays/gammas. alphas. Am-Pu-Cm source. Voltage [mv] Voltage [mv]
Development of CdZnTe for use as a tool in Nuclear Spectroscopy: GR/ M37325/1 Review Report October 1998 { October 2 1. BACKGROUND This fast track grant was aimed at the development of the semiconductor
More informationGeorgia Institute of Technology. Radiation Detection & Protection (Day 3)
Georgia Institute of Technology The George W. Woodruff School of Mechanical Engineering Nuclear & Radiological Engineering/Medical Physics Program Ph.D. Qualifier Exam Spring Semester 2009 Your ID Code
More informationEEE4106Z Radiation Interactions & Detection
EEE4106Z Radiation Interactions & Detection 2. Radiation Detection Dr. Steve Peterson 5.14 RW James Department of Physics University of Cape Town steve.peterson@uct.ac.za May 06, 2015 EEE4106Z :: Radiation
More informationGeant4 simulation of SOI microdosimetry for radiation protection in space and aviation environments
Geant4 simulation of SOI microdosimetry for radiation protection in space and aviation environments Dale A. Prokopovich,2, Mark I. Reinhard, Iwan M. Cornelius 3 and Anatoly B. Rosenfeld 2 Australian Nuclear
More informationA Monte Carlo Simulation for Estimating of the Flux in a Novel Neutron Activation System using 252 Cf Source
IOSR Journal of Applied Physics (IOSR-JAP) e-issn: 2278-4861.Volume 7, Issue 3 Ver. II (May. - Jun. 2015), PP 80-85 www.iosrjournals.org A Monte Carlo Simulation for Estimating of the Flux in a Novel Neutron
More informationComparison of the Photo-peak Efficiencies between the Experimental Data of 137 Cs Radioactive Source with Monte Carlo (MC) Simulation Data
International Journal of Advanced Research in Physical Science (IJARPS) Volume 5, Issue 10, 2018, PP 24-28 ISSN No. (Online) 2349-7882 www.arcjournals.org Comparison of the Photo-peak Efficiencies between
More informationPhotoneutron reactions studies at ELI-NP using a direct neutron multiplicity sorting method Dan Filipescu
EUROPEAN UNION GOVERNMENT OF ROMANIA Sectoral Operational Programme Increase of Economic Competitiveness Investments for Your Future Structural Instruments 2007-2013 Extreme Light Infrastructure Nuclear
More informationBasic hands-on gamma calibration for low activity environmental levels
Basic hands-on gamma calibration for low activity environmental levels Iolanda Osvath Presented by Mats Eriksson Environment Laboratories Marine Environment Laboratories, Monaco Radiometrics Laboratory
More informationPhotoneutron Interrogation of Uranium Samples by a 4 MeV LINAC. A Feasibility Study
Photoneutron Interrogation of Uranium Samples by a 4 MeV LINAC. A Feasibility Study L. Lakosi, C. T. Nguyen, J. Bagi Institute of Isotopes, Hungarian Academy of Sciences P. O. Box 77, H-1525 Budapest,
More informationMITOCW watch?v=wr88_vzfcx4
MITOCW watch?v=wr88_vzfcx4 PROFESSOR: So we're building this story. We had the photoelectric effect. But at this moment, Einstein, in the same year that he was talking about general relativity, he came
More informationPrompt gamma measurements for the verification of dose deposition in proton therapy. Contents. Two Proton Beam Facilities for Therapy and Research
Prompt gamma measurements for the verification of dose deposition in proton therapy Two Proton Beam Facilities for Therapy and Research Ion Beam Facilities in Korea 1. Proton therapy facility at National
More informationNuclear Reactions A Z. Radioactivity, Spontaneous Decay: Nuclear Reaction, Induced Process: x + X Y + y + Q Q > 0. Exothermic Endothermic
Radioactivity, Spontaneous Decay: Nuclear Reactions A Z 4 P D+ He + Q A 4 Z 2 Q > 0 Nuclear Reaction, Induced Process: x + X Y + y + Q Q = ( m + m m m ) c 2 x X Y y Q > 0 Q < 0 Exothermic Endothermic 2
More informationCopyright 2008, University of Chicago, Department of Physics. Gamma Cross-sections. NaI crystal (~2" dia) mounted on photo-multiplier tube
Gamma Cross-sections 1. Goal We wish to measure absorption cross-sections for γ-rays for a range of gamma energies and absorber atomic number. 2. Equipment Pulse height analyzer Oscilloscope NaI crystal
More informationCOMPTON imaging is an attractive technology used in
1 Experimental results of the gamma-ray imaging capability with a Si/CdTe semiconductor Compton camera Shin ichiro Takeda, Hiroyuki Aono, Sho Okuyama, Shin-nosuke Ishikawa, Hirokazu Odaka, Shin Watanabe,
More informationIntroduction CHAPTER 01. Light and opto-semiconductors. Opto-semiconductor lineup. Manufacturing process of opto-semiconductors.
CHAPTER 0 Light and opto-semiconductors - -2 Light Opto-semiconductors P. 0 P. 3 2 Opto-semiconductor lineup P. 5 3 Manufacturing process of opto-semiconductors P. 6 9 CHAPTER 0. Light and opto-semiconductors
More informationAttenuation of Radiation in Matter. Attenuation of gamma particles
Attenuation of Radiation in Matter In this experiment we will examine how radiation decreases in intensity as it passes through a substance. Since radiation interacts with matter, its intensity will decrease
More informationJournal of Chemical and Pharmaceutical Research, 2012, 4(1): Research Article
Available online www.jocpr.com Journal of Chemical and Pharmaceutical Research, 212, 4(1):118-124 Research Article ISSN : 975-7384 CODEN(USA) : JCPRC5 Photon interaction cross-section of elemental solids
More information