Physics in Nuclear Medicine

Size: px
Start display at page:

Download "Physics in Nuclear Medicine"

Transcription

1 SIMON R. CHERRY, PH.D. Professor Department of Biomedical Engineering University of California-Davis Davis, California JAMES A. SORENSON, PH.D. Emeritus Professor of Medical Physics University of Wisconsin-Madison Madison, Wisconsin MICHAEL E. PHELPS, PH. D. Norton Simon Professor Chair, Department of Molecular and Medical Pharmacology Director, Center for Molecular Medicine Director, Crump Institute for Molecular Imaging David Geffen School of Medicine, UCLA Los Angeles, California Physics in Nuclear Medicine third edition SAUNDERS :4r : Imprint of Elsevier

2 What Is Nuclear Medicine? 1 G. Positron (R+) and (R+, ~,) Decay 25 A. Fundamental Concepts 1 H. Competitive R+ B. The and EC Decay Power of Nuclear Medicine 27 1 I, Decay by a Emission C. Historical Overview 2 and by Nuclear Fission 2'7 D. Current Practice of Nuclear J. Decay Medicine Modes and the Line of 3 E. Stability 28 The Role of Physics in Nuclear K. Sources of Medicine 6 Information on Radionuclides 30 Basic Atomic and Nuclear Physics 7 (1) Decay of Radioactivity 31 A. Quantities and Units 7 1. Types of Quantities and Units 7 A. Activity Mass and Energy Units 7 1. The Decay Constant 31 B. Radiation 8 2. Definition and Units of Activity 31 C. Atoms 9 B. Exponential Decay Composition and Structure 9 1. The Decay Factor Electron Binding Energies and 2. Half-Life 33 Energy Levels Average Lifetime Atomic Emissions 11 C. Methods for Determining Decay D. The Nucleus 13 Factors Composition Tables of Decay Factors Terminology and Notation Pocket Calculators Nuclear Families Graphic Methods Forces and Energy Levels within the D. Image-Frame Decay Corrections 36 Nucleus 14 E. Specific Activity Nuclear Emissions 16 F. Decay of a Mixed Radionuclide 6. Nuclear Binding Energy Characteristics of Stable Sample 40 Nuclei 16 G. Parent-Daughter Decay The Bateman Equations 41 Modes of Radioactive 2. Secular Equilibrium 41 Decay Transient Equilibrium No Equilibrium 43 A. General Concepts 19 B. Chemistry and Radioactivity 19 C. Decay by R_ Emission 20 D. Decay by (0-,,y) Emission 22 Radionuclide and E. Isomeric Transition (IT) and Internal Radiopharmaceutical Conversion Production 45 (IC) 23 F. Electron Capture (EC) and (EC, y) A. Reactor-Produced Radionuclides 45 Decay Reactor Principles 45

3 viii... PHYSICS IN NUCLEAR MEDICINE 2. Fission Fragments Neutron Activation 48 B. Accelerator-Produced Radionuclides Charged-Particle Accelerators Cyclotron Principles Cyclotron-Produced Radionuclides 51 C. Radionuclide Generators 52 D. Equations for Radionuclide Production Activation Cross Sections Activation Rates Buildup and Decay of Activity 57 E. Radionuclides for Nuclear Medicine General Considerations Specific Considerations 59 F. Radiopharmaceutical Preparation General Considerations Labeling Strategies Technetium 99m-Labeled Radiopharmaceuticals Radiopharmaceuticals Labeled with Positron Emitters Radiopharmaceuticals for Therapy Applications Radiopharmaceuticals in Clinical Nuclear Medicine 63 Interaction of Radiation with Matter 65 A. Interactions of Charged Particles with Matter Charged-Particle Interaction Mechanisms Collisional Versus Radiation Losses Charged-Particle Tracks Deposition of Energy Along a Charged-Particle Track The Cerenkov Effect 71 B. Charged-Particle Ranges Alpha Particles Beta Particles and Electrons 74 C. Passage of High-Energy Photons through Matter Photon Interaction Mechanisms The Photoelectric Effect Compton Scattering Pair Production Coherent (Rayleigh) Scattering Deposition of Photon Energy in Matter 80 D. Attenuation of Photon Beams Attenuation Coefficients Thick Absorbers, Narrow-Beam Geometry Thick Absorbers, Broad-Beam Geometry Polyenergetic Sources 88 Radiation Detectors 89 A. Gas-Filled Detectors Basic Principles Ionization Chambers Proportional Counters Geiger-Muller Counters 94 B. Semiconductor Detectors 98 C. Scintillation Detectors Basic Principles Photomultiplier Tubes Inorganic Scintillators Organic Liquid Scintillators 106 Electronic Instrumentation for Radiation Detection Systems 109 A. Preamplifiers 109 B. Amplifiers Amplification and Pulse-Shaping Functions Resistor-Capacitor Shaping Baseline Shift and Pulse Pile-up 114 C. Pulse-Height Analyzers Basic Functions Single-Channel Analyzers Timing Methods Multichannel Analyzers 117 D. Time-to-Amplitude Converters 121 E. Digital Counters and Rate Meters Scalers, Timers, and Counters Analog Rate Meters 123 F. Coincidence Units 124 G. High-Voltage Power Supplies 125 H. Nuclear Instrument Modules 126 I. Cathode Ray Tube Electron Gun Deflection Plates Phosphor-Coated Display Screens Focus and Brightness Controls Color Cathode Ray Tubes 128

4 J. Oscilloscopes Semiconductor Detector K. Computer Monitors 129 Spectrometers Liquid Scintillation Spectrometry Proportional Counter Nuclear Counting Statistics 131 Spectrometers 163 A. Types of Measurement Error 131 B. Nuclear Counting Statistics The Poisson Distribution The Standard Deviation The Gaussian Distribution 134 Problems in Radiation Detection and Measurement 165 A. Detection Efficiency 165 C. Propagation of Errors Components of Detection 1. Sums and Differences 135 Efficiency Constant Multipliers Geometric Efficiency Products and Ratios Intrinsic Efficiency More Complicated 4. Energy Selective Counting 169 Combinations Some Complicating Factors 170 D. Applications of Statistical 6. Calibration Sources 175 Analysis 136 B. Problems in the Detection and 1. Effects of Averaging 136 Measurement of R Particles Counting Rates 137 C. Dead Time 3. Significance of Differences 1. between Counting Causes of Dead Time Measurements 137 Mathematical Models Effects of Background 3. Window Fraction 137 Effects Minimum 4. Dead Time Detectable Activity 138 Correction Methods 181 D. 6. Comparing Counting Quality Assurance for Radiation Systems 138 Measurement Systems Estimating Required Counting Times Optimal Division of Counting Times 140 Counting Systems 185 E. Statistical Tests 140 A. Nal(TI) Well Counter The X2 Test Detector Characteristics The t-test Detection Efficiency Treatment of "Outliers" Sample Volume Effects 188 Contents** e ix 4. Linear Regression Assay of Absolute Activity Shielding and Background Energy Calibration 191 Pulse-Height Spectrometry Multiple Radionuclide Source Counting 191 A. Basic Principles Dead Time 192 B. Spectrometry with Nal(TI) Automatic Multiple-Sample 1. The Ideal Pulse-Height Systems 192 Spectrum Applications The Actual Spectrum 151 B. Counting with Conventional Nal(TI) 3. Effects of Detector Size 154 Detectors Effects of Counting Rate Large Sample Volumes General Effects of r-ray 2. Liquid and Gas Flow Energy 155 Counting Energy Linearity 157 C. Liquid Scintillation Counters Energy Resolution General Characteristics 196 C. Spectrometry with Other 2. Pulse-Height Spectrometry 198 Detectors Counting Vials 198

5 x.. * PHYSICS IN NUCLEAR MEDICINE 4. Energy and Efficiency Calibrations Quench Corrections Sample Preparation Techniques Liquid and Gas Flow Counting Automatic Multiple-Sample LS Counters Applications 202 D. Gas-Filled Detectors Dose Calibrators Gas Flow Counters 204 E. Semiconductor Detector Systems System Components Applications 207 F. In Vivo Counting Systems Nal(TI) Probe Systems Miniature 7-Ray Probes for Surgical Use Whole-Body Counters 210 The Gamma Camera : Basic Principles 211 C. D. E. 2. Image Nonuniformity Nonuniformity Correction Techniques Gamma Camera Tuning 238 Design and Performance Characteristics of Parallel-Hole Collimators Basic Limitations in Collimator Performance Spatal Thickness Geometry of Collimator Holes System Resolution 244 Performance Characteristics of Converging, Diverging, and Pinhole Collimators 245 Measurements of Gamma Camera Performance Intrinsic Resolution System Resolution Spatial Linearity Uniformity Counting Rate Performance Energy Resolution System Sensitivity 250 A. General Concepts of Radionuclide Image Quality in Imaging 211 Nuclear Medicine 253 B. Basic Principles of the Gamma Camera 212 A. Basic Methods for Characterizing Components and Evaluating..-_ " _ and Q Electronics 213 B. Spatial Resolution Collimators Factors Affecting Spatial " " Gamma " - Camera Methods for Evaluating Spatial C. Types of Gamma Cameras and Resolution 254 Their Clinical Uses 223 C. Contrast 259 -Noise 263 The Gamma Camera : Performance " - " Image Noise Random Noise "" Contrast-to-Noise Ratio Characteristics 227 E. Observer Performance Studies 268 A. Basic Performance 1. Contrast-Detail (C-D) Studies Receiver Operating Characteristic Characteristics 227 (ROC) Studies Intrinsic Spatial Resolution Detection Efficiency Energy Resolution 230 Tomographic 4. Performance at High Counting Reconstruction Rates 231 in Nuclear Medicine B. 273 Detector Limitations : Nonuniformity and Nonlinearity 234 A. General Concepts, Notation, and 1. Image Nonlinearity 234 Terminology 274

6 B. Backprojection and Fourier-Based Positron Emission Techniques 276 Tomography Simple Backprojection Direct Fourier Transform A. Annihilation Coincidence Reconstruction 278 Detection Filtered Backprojection Basic Principles of Annihilation 4. Multislice Imaging 283 Coincidence Detection 325 C. Image Quality in Fourier Transform 2. Time-of-Flight PET 327 and Filtered Backprojection 3. Spatial Resolution : Detectors Spatial Resolution : Positron Techniques 283 Physics Effects of Sampling on Image 5. Spatial Resolution : Quality 283 Depth-of-Interaction Effect Sampling Coverage and 6. Spatial Resolution : Sampling 336 Consistency Requirements Spatial Resolution : 3. Noise Propagation, Signal-to-Noise Reconstruction Filters 336 Ratio, and Contrast-to-Noise 8. Sensitivity 337 Ratio Event Types in Annihilation D. Iterative Reconstruction Coincidence Detection 340 Algorithms 291 B. PET Detector and Scanner 1. General Concepts of Iterative Designs 342 Reconstruction Block Detectors Expectation-Maximization 2. Modified Block Detectors 344 Reconstruction Dedicated PET Systems 346 E. Reconstruction of Fan-Beam and 4. Gamma Camera Systems Cone-Beam Data 294 for PET 348 C. Data Acquisition for PET Two-Dimensional Data Single Photon Emission Computed Tomography 299 Acquisition Three-Dimensional Data Acquisition Data Acquisition for Dynamic A. SPECT Systems 299 Studies and Whole-Body 1. Gamma Camera Scans 353 SPECT Systems 299 D. Data Corrections and 2. Advanced SPECT Systems Combined Modality Systems 302 B. Practical Implementation Quantitative Aspects of PET Normalization 353 2~ Correction for Random Coincidences 354 of SPECT Correction for Scattered 1. Attenuation Effects Radiation 355 and Conjugate Counting Attenuation Correction Attenuation Correction Dead Time Corrections Transmission Scans and Attenuation 6. Absolute Quantification of Maps 313 PET Images Scatter Corrections 315 E. Clinical and Research 5. Partial-Volume Effects 317 Applications of PET 358 Contents o o 9 xi C. Performance Characteristics of SPECT Systems Spatial Resolution Volume Sensitivity 320 Digital Image Processing in 3. Other Measurements of Nuclear Medicine 361 Performance Quality Assurance in SPECT 321 A. Digital Images 362 D. Clinical Applications of 1. Basic Characteristics and SPECT 322 Terminology 362

7 xii. * * PHYSICS IN NUCLEAR MEDICINE 2. Spatial Resolution and Matrix Size Image Display Acquisition Modes 366 B. Digital Image-Processing Techniques Image Visualization Regions and Volumes of Interest Time-Activity Curves Image Smoothing Edge Detection and Segmentation Co-registration of Images 373 C. Processing Environment 375 Tracer Kinetic Modeling 377 A. Basic Concepts 377 B. Tracers and Compartments Definition of a Tracer Definition of a Compartment Distribution Volume and Partition Coefficient Flux Rate Constants Steady State 383 C. Tracer Delivery and Transport Blood Flow, Extraction, and Clearance Transport 387 D. Formulation of a Compartmental Model 388 E. Examples of Dynamic Imaging and Tracer Kinetic Models Cardiac Function and Ejection Fraction Blood Flow Models Blood Flow : Trapped Radiotracers Blood Flow : Clearance Techniques Enzyme Kinetics : Glucose Metabolism Receptor Ligand Assays 401 F. Summary 402 Internal Radiation Dosimetry 405 A. Radiation Dose and Equivalent Dose : Quantities and Units 405 B. Calculation of Radiation Dose (MIRD Method) Basic Procedure and Some Practical Problems Cumulated Activity, A Equilibrium Absorbed Dose Constant, A Absorbed Fraction, ~ Specific Absorbed Fraction, (D, and the Dose Reciprocity Theorem Mean Dose per Cumulated Activity, S Whole-Body Dose, Effective Dose, and Effective Dose Equivalent Limitations of the MIRD Method 417 Radiation Safety and Health Physics 427 A. Quantities and Units Dose-Modifying Factors Exposure and Air Kerma 428 B. Regulations Pertaining to the Use of Radionuclides Nuclear Regulatory Commission Licensing and Regulations Restricted and Unrestricted Areas Dose Limits Concentrations for Airborne Radioactivity in Restricted Areas Environmental Concentrations and Concentrations for Sewage Disposal Record-Keeping Requirements Recommendations of Advisory Bodies 432 C. Safe Handling of Radioactive Materials The ALARA Concept Reduction of Radiation Doses from External Sources Reduction of Radiation Doses from Internal Sources Laboratory Design Procedures for Handling Spills 438 D. Disposal of Radioactive Waste 439 E. Radiation Monitoring Survey Meters and Laboratory Monitors 439

8 2. Personnel Dosimeters Wipe Testing 440 Appendix A: Unit Conversions 443 Appendix 8: Properties of the Elements 444 Contents + s * Ail Appendix E: Effective Dose Equivalent (msv/mbq) and Radiation Absorbed Dose Estimates (mgy/mbq) to Adult Subjects from Selected Internally Administered Radiopharmaceuticals 480 Appendix C: Characteristics of Some Medically Appendix F: The Fourier Transform 483 Important A. The FT: What It Radionuclides Represents B. Calculating FTs 484 Appendix D: Mass Attenuation C. Some Properties of FTs 485 Coefficients for Water, D. Some Examples of FTs 488 Sodium Iodide, BGO, CZT, Appendix G: Convolutions 493 and Lead 479 Index 499

Radiation Detection and Measurement

Radiation Detection and Measurement Radiation Detection and Measurement June 2008 Tom Lewellen Tkldog@u.washington.edu Types of radiation relevant to Nuclear Medicine Particle Symbol Mass (MeV/c 2 ) Charge Electron e-,! - 0.511-1 Positron

More information

Radionuclide Imaging MII Positron Emission Tomography (PET)

Radionuclide Imaging MII Positron Emission Tomography (PET) Radionuclide Imaging MII 3073 Positron Emission Tomography (PET) Positron (β + ) emission Positron is an electron with positive charge. Positron-emitting radionuclides are most commonly produced in cyclotron

More information

Outline Chapter 14 Nuclear Medicine

Outline Chapter 14 Nuclear Medicine Outline Chapter 14 uclear Medicine Radiation Dosimetry I Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4 th ed. http://www.utoledo.edu/med/depts/radther Introduction Detectors for nuclear

More information

MEASUREMENT AND DETECTION OF RADIATION

MEASUREMENT AND DETECTION OF RADIATION MEASUREMENT AND DETECTION OF RADIATION Second Edition Nicholas Tsoulfanidis University of Missouri-Rolla Ж Taylor &Francis * Publishers since I79H CONTENTS Preface to the First Edition Preface to the Second

More information

APPLIED RADIATION PHYSICS

APPLIED RADIATION PHYSICS A PRIMER IN APPLIED RADIATION PHYSICS F A SMITH Queen Mary & Westfield College, London fe World Scientific m Singapore * New Jersey London Hong Kong CONTENTS CHAPTER 1 : SOURCES of RADIATION 1.1 Introduction

More information

MEDICAL EQUIPMENT: NUCLEAR MEDICINE. Prof. Yasser Mostafa Kadah

MEDICAL EQUIPMENT: NUCLEAR MEDICINE. Prof. Yasser Mostafa Kadah MEDICAL EQUIPMENT: NUCLEAR MEDICINE Prof. Yasser Mostafa Kadah www.k-space.org Recommended Textbook Introduction to Medical Imaging: Physics, Engineering and Clinical Applications, by Nadine Barrie Smith

More information

There are three mechanisms by which gamma rays interact with absorber atoms from which two are important for nuclear medicine.

There are three mechanisms by which gamma rays interact with absorber atoms from which two are important for nuclear medicine. Measurement of radioactivity. Radioactive decay is a random process and therefore fluctuations are expected in the radioactivity measurement. That is why measurement of radioactivity must be treated by

More information

Michael G. Stabin. Radiation Protection and Dosimetry. An Introduction to Health Physics. 4) Springer

Michael G. Stabin. Radiation Protection and Dosimetry. An Introduction to Health Physics. 4) Springer Michael G. Stabin Radiation Protection and Dosimetry An Introduction to Health Physics 4) Springer Table of Contents Preface Acknowledgments Chapter 1. Introduction to Health Physics 1 1.1 Definition of

More information

EEE4106Z Radiation Interactions & Detection

EEE4106Z 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 information

PHYSICS FOR RADIATION PROTECTION

PHYSICS FOR RADIATION PROTECTION PHYSICS FOR RADIATION PROTECTION JAMES E. MARTIN School of Public Health The University of Michigan A Wiley-Interscience Publication JOHN WILEY & SONS, INC. New York Chichester Weinheim Brisbane Singapore

More information

Radiation Detectors. How do we detect ionizing radiation? What are these effects? Types of Ionizing Radiation Detectors

Radiation Detectors. How do we detect ionizing radiation? What are these effects? Types of Ionizing Radiation Detectors Radiation Detectors 1 How do we detect ionizing radiation? Indirectly, by its effects as it traverses matter? What are these effects? Ionization and excitation of the atoms and molecules Heat 2 Types of

More information

UNCORRECTED PROOF. Table of Contents

UNCORRECTED PROOF. Table of Contents 00-Stabin-Prelims SNY001-Stabin (Typeset by spi publisher services, Delhi) vii of xvi June 1, 2007 17:15 Preface xiii Acknowledgments xv Chapter 1. Introduction to Health Physics 1 1.1 Definition of Health

More information

Nuclear Medicine Intro & Physics from Medical Imaging Signals and Systems, Chapter 7, by Prince and Links

Nuclear Medicine Intro & Physics from Medical Imaging Signals and Systems, Chapter 7, by Prince and Links Nuclear Medicine Intro & Physics from Medical Imaging Signals and Systems, Chapter 7, by Prince and Links NM - introduction Relies on EMISSION of photons from body (versus transmission of photons through

More information

Atoms, Radiation, and Radiation Protection

Atoms, Radiation, and Radiation Protection James E. Turner Atoms, Radiation, and Radiation Protection Third, Completely Revised and Enlarged Edition BICENTENNIAL J 0 1 8 0 Q 71 z m z CAVILEY 2007 1 ;Z z ü ; m r B10ENTENNIAL WILEY-VCH Verlag GmbH

More information

Interactions of Radiation with Matter

Interactions of Radiation with Matter Main points from last week's lecture: Decay of Radioactivity Mathematics description nly yields probabilities and averages Interactions of Radiation with Matter William Hunter, PhD" Decay equation: N(t)

More information

What is scintigraphy? The process of obtaining an image or series of sequential images of the distribution of a radionuclide in tissues, organs, or

What is scintigraphy? The process of obtaining an image or series of sequential images of the distribution of a radionuclide in tissues, organs, or Let's remind... What is nuclear medicine? Nuclear medicine can be broadly divided into two branches "in vitro" and "in vivo" procedures. There are numerous radioisotopic "in vitro" procedures for genotyping

More information

Medical Physics. Nuclear Medicine Principles and Applications

Medical Physics. Nuclear Medicine Principles and Applications Medical Physics Nuclear Medicine Principles and Applications Dr Roger Fulton Department of PET & Nuclear Medicine Royal Prince Alfred Hospital Sydney Email: rfulton@mail.usyd.edu.au Lectures: http://www-personal.usyd.edu.au/~rfulton/medical_physics

More information

Radiation Detection and Measurement

Radiation Detection and Measurement Radiation Detection and Measurement Fourth Edition Glenn F. Knoll Professor Emeritus of Nuclear Engineering and Radiological Sciences University of Michigan Ann Arbor, Michigan WILEY John Wiley & Sons,

More information

Radiation Detection and Measurement

Radiation Detection and Measurement Radiation Detection and Measurement Third Edition Glenn F. Knoll Professor of Nuclear Engineering and Radiological Sciences University of Michigan Ann Arbor, Michigan John Wiley & Sons, Inc. New York/Chichester/Weinheim/Brisbane/Toronto/Singapore

More information

Contents. Charged Particles. Coulomb Interactions Elastic Scattering. Coulomb Interactions - Inelastic Scattering. Bremsstrahlung

Contents. Charged Particles. Coulomb Interactions Elastic Scattering. Coulomb Interactions - Inelastic Scattering. Bremsstrahlung Contents Marcel MiGLiERiNi Nuclear Medicine, Radiology and Their Metrological Aspects. Radiation in Medicine. Dosimetry 4. Diagnostics & Therapy 5. Accelerators in Medicine 6. Therapy Planning 7. Nuclear

More information

RPR 29 CYCLOTRON RADIOCHEMISTRY LABORATORY

RPR 29 CYCLOTRON RADIOCHEMISTRY LABORATORY RPR 29 CYCLOTRON RADIOCHEMISTRY LABORATORY PURPOSE This procedure provides instructions for developing, maintaining, and documenting, radiation safety procedures conducted at the Cyclotron Radiochemistry

More information

A. I, II, and III B. I C. I and II D. II and III E. I and III

A. I, II, and III B. I C. I and II D. II and III E. I and III BioE 1330 - Review Chapters 7, 8, and 9 (Nuclear Medicine) 9/27/2018 Instructions: On the Answer Sheet, enter your 2-digit ID number (with a leading 0 if needed) in the boxes of the ID section. Fill in

More information

Radionuclide Imaging MII Detection of Nuclear Emission

Radionuclide Imaging MII Detection of Nuclear Emission Radionuclide Imaging MII 3073 Detection of Nuclear Emission Nuclear radiation detectors Detectors that are commonly used in nuclear medicine: 1. Gas-filled detectors 2. Scintillation detectors 3. Semiconductor

More information

GLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY

GLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY GLOSSARY OF BASIC RADIATION PROTECTION TERMINOLOGY ABSORBED DOSE: The amount of energy absorbed, as a result of radiation passing through a material, per unit mass of material. Measured in rads (1 rad

More information

Decay of Radioactivity

Decay of Radioactivity Decay of Radioactivity Robert Miyaoka, PhD rmiyaoka@u.washington.edu Nuclear Medicine Basic Science Lectures September 15, 2015 Review of last week: Introduction to Nuclear Physics and Nuclear Decay Nuclear

More information

Fundamentals of Radionuclide Metrology

Fundamentals of Radionuclide Metrology Fundamentals of Radionuclide Metrology Brian E. Zimmerman, PhD Physical Measurement Laboratory National Institute of Standards and Technology Gaithersburg, MD USA SIM Metrology Workshop Buenos Aires, Argentina

More information

Mitigation of External Radiation Exposures

Mitigation of External Radiation Exposures Mitigation of External Radiation Exposures The three (3) major principles to assist with maintaining doses ALARA are :- 1) Time Minimizing the time of exposure directly reduces radiation dose. 2) Distance

More information

RADIATION DETECTION AND MEASUREMENT

RADIATION DETECTION AND MEASUREMENT RADIATION DETECTION AND MEASUREMENT SECOND EDITION GLENN F. KNOLL Professor of Nuclear Engineering The University of Michigan Ann Arbor, Michigan WILEY JOHN WILEY & SONS New York Chichester Brisbane Toronto

More information

Acronyms, Abbreviations, and Symbols Foreword to the First Edition Foreword to the Second Edition Preface to the First Edition Preface to the Second

Acronyms, Abbreviations, and Symbols Foreword to the First Edition Foreword to the Second Edition Preface to the First Edition Preface to the Second Contributors p. xxix Acronyms, Abbreviations, and Symbols p. xxxi Foreword to the First Edition p. xliii Foreword to the Second Edition p. xlv Preface to the First Edition p. xlvii Preface to the Second

More information

Dosimetry of patients injected with tracers Ga-68, Zr-89 and Lu-177. Bruno Vanderlinden

Dosimetry of patients injected with tracers Ga-68, Zr-89 and Lu-177. Bruno Vanderlinden Dosimetry of patients injected with tracers Ga-68, Zr-89 and Lu-177 Bruno Vanderlinden What is NM speciality? Imaging radiology Physics Diagnostic Treatment assessment Clinical pathology Biological marker

More information

1st Faculty of Medicine, Charles University in Prague Center for Advanced Preclinical Imaging (CAPI)

1st Faculty of Medicine, Charles University in Prague Center for Advanced Preclinical Imaging (CAPI) Radioation Resolution and Sensitivity Nuclear Imaging PET + SPECT Radioactive Decay (EC,Ɣ), (β -,Ɣ), (I.T.,Ɣ) β + Projection imaging collimator needed one angular view Projection imaging coincidence imaging,

More information

PHYSICS A2 UNIT 2 SECTION 1: RADIOACTIVITY & NUCLEAR ENERGY

PHYSICS A2 UNIT 2 SECTION 1: RADIOACTIVITY & NUCLEAR ENERGY PHYSICS A2 UNIT 2 SECTION 1: RADIOACTIVITY & NUCLEAR ENERGY THE ATOMIC NUCLEUS / NUCLEAR RADIUS & DENSITY / PROPERTIES OF NUCLEAR RADIATION / INTENSITY & BACKGROUND RADIATION / EXPONENTIAL LAW OF DECAY

More information

Introduction to SPECT & PET TBMI02 - Medical Image Analysis 2017

Introduction to SPECT & PET TBMI02 - Medical Image Analysis 2017 Introduction to SPECT & PET TBMI02 - Medical Image Analysis 2017 Marcus Ressner, PhD, Medical Radiation Physicist, Linköping University Hospital Content What is Nuclear medicine? Basic principles of Functional

More information

Theoretical questions for the final exam ED 2012.

Theoretical questions for the final exam ED 2012. Theoretical questions for the final exam ED 2012. 1. Radiation a) Properties and types of radiation b) Physical parameters of radiation 2. Law of attenuation of radiation a) Experimental interpretation

More information

Foundation of Radiological Physics. Preface

Foundation of Radiological Physics. Preface Foundation of Radiological Physics Page Preface v Chapter 1. Radiation 1 1.1 Medical Use of Radiation. 1 1.2 Nature of Radiation. 4 1.3 Quantum Nature of Radiation. 6 1.4 Electromagnetic Radiation Spectrum

More information

Lecture Presentation. Chapter 21. Nuclear Chemistry. James F. Kirby Quinnipiac University Hamden, CT Pearson Education, Inc.

Lecture Presentation. Chapter 21. Nuclear Chemistry. James F. Kirby Quinnipiac University Hamden, CT Pearson Education, Inc. Lecture Presentation Chapter 21, Inc. James F. Kirby Quinnipiac University Hamden, CT Energy: Chemical vs. Chemical energy is associated with making and breaking chemical bonds. energy is enormous in comparison.

More information

DETECTORS. I. Charged Particle Detectors

DETECTORS. I. Charged Particle Detectors DETECTORS I. Charged Particle Detectors A. Scintillators B. Gas Detectors 1. Ionization Chambers 2. Proportional Counters 3. Avalanche detectors 4. Geiger-Muller counters 5. Spark detectors C. Solid State

More information

6: Positron Emission Tomography

6: Positron Emission Tomography 6: Positron Emission Tomography. What is the principle of PET imaging? Positron annihilation Electronic collimation coincidence detection. What is really measured by the PET camera? True, scatter and random

More information

Radiochemistry and Nuclear Methods of Analysis

Radiochemistry and Nuclear Methods of Analysis Radiochemistry and Nuclear Methods of Analysis WILLIAM D. EHMANN Professor, Department of Chemistry University of Kentucky Lexington, Kentucky DIANE E. VANCE Staff Development Scientist Analytical Services

More information

QUIZ: 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 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 information

Chemical Engineering 412

Chemical 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 information

A Brief Introduction to Medical Imaging. Outline

A Brief Introduction to Medical Imaging. Outline A Brief Introduction to Medical Imaging Outline General Goals Linear Imaging Systems An Example, The Pin Hole Camera Radiations and Their Interactions with Matter Coherent vs. Incoherent Imaging Length

More information

Detection and measurement of gamma-radiation by gammaspectroscopy

Detection and measurement of gamma-radiation by gammaspectroscopy Detection and measurement of gamma-radiation by gammaspectroscopy Gamma-radiation is electromagnetic radiation having speed equal to the light in vacuum. As reaching a matter it interact with the different

More information

Chapter 2 PET Imaging Basics

Chapter 2 PET Imaging Basics Chapter 2 PET Imaging Basics Timothy G. Turkington PET Radiotracers Positron emission tomography (PET) imaging is the injection (or inhalation) of a substance containing a positron emitter, the subsequent

More information

Radiation Protection & Radiation Therapy

Radiation Protection & Radiation Therapy Radiation Protection & Radiation Therapy For Medical Students Professor of Medical Physics Radiation Units Activity Number disintegrations per second (Curie, Becquerel) Exposure (Roentgen, C/kg) Absorbed

More information

Scintillation Detector

Scintillation Detector Scintillation Detector Introduction The detection of ionizing radiation by the scintillation light produced in certain materials is one of the oldest techniques on record. In Geiger and Marsden s famous

More information

Interaction of charged particles and photons with matter

Interaction of charged particles and photons with matter Interaction of charged particles and photons with matter Robert Miyaoka, Ph.D. Old Fisheries Center, Room 200 rmiyaoka@u.washington.edu Passage of radiation through matter depends on Type of radiation

More information

Nuclear and Radiochemistry

Nuclear and Radiochemistry Nuclear and Radiochemistry Third Edition Gerhart Friedlander Senior Chemist, Brookhaven National Laboratory Joseph W. Kennedy Late Professor of Chemistry, Washington University, St. Louis Edward S. Macias

More information

Basic physics Questions

Basic physics Questions Chapter1 Basic physics Questions S. Ilyas 1. Which of the following statements regarding protons are correct? a. They have a negative charge b. They are equal to the number of electrons in a non-ionized

More information

Dana-Farber Cancer Institute, 44 Binney Street, Boston, MA 02115, USA ramsey

Dana-Farber Cancer Institute, 44 Binney Street, Boston, MA 02115, USA   ramsey SPECIAL FEATURE: MEDICAL PHYSICS www.iop.org/journals/physed Nuclear medicine Ramsey D Badawi Dana-Farber Cancer Institute, 44 Binney Street, Boston, MA 02115, USA E-mail: ramsey badawi@dfci.harvard.edu

More information

Structure of Biological Materials

Structure of Biological Materials ELEC ENG 3BA3: Structure of Biological Materials Notes for Lecture #19 Monday, November 22, 2010 6.5 Nuclear medicine imaging Nuclear imaging produces images of the distribution of radiopharmaceuticals

More information

O WILEY- MODERN NUCLEAR CHEMISTRY. WALTER D. LOVELAND Oregon State University. DAVID J. MORRISSEY Michigan State University

O WILEY- MODERN NUCLEAR CHEMISTRY. WALTER D. LOVELAND Oregon State University. DAVID J. MORRISSEY Michigan State University MODERN NUCLEAR CHEMISTRY WALTER D. LOVELAND Oregon State University DAVID J. MORRISSEY Michigan State University GLENN T. SEABORG University of California, Berkeley O WILEY- INTERSCIENCE A JOHN WILEY &

More information

Detector technology. Aim of this talk. Principle of a radiation detector. Interactions of gamma photons (gas) Gas-filled detectors: examples

Detector technology. Aim of this talk. Principle of a radiation detector. Interactions of gamma photons (gas) Gas-filled detectors: examples Aim of this tal Detector technology WMIC Educational Program Nuclear Imaging World Molecular Imaging Congress, Dublin, Ireland, Sep 5-8, 202 You can now the name of a bird in all the languages of the world,

More information

Final exam questions ED

Final exam questions ED Final exam questions ED 2015-2016 1. Radiation a) Properties and types of radiation b) Physical parameters of radiation 2. Law of attenuation of radiation a) Experimental interpretation of the law b) Forms

More information

Compton Camera. Compton Camera

Compton 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 information

Activities at the Laboratory of the Nuclear Engineering Department of the Polytechnic University of Valencia

Activities at the Laboratory of the Nuclear Engineering Department of the Polytechnic University of Valencia 7 th Workshop on European Collaboration for Higher Education and Research in Nuclear Engineering & Radiological Protection Bruxelles, Belgique 30 May - 1 June 2011 Activities at the Laboratory of the Nuclear

More information

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous?

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous? Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous? 2. Briefly discuss dead time in a detector. What factors are important

More information

Chapter Seven (Nuclear Detectors)

Chapter 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 information

Basic physics of nuclear medicine

Basic physics of nuclear medicine Basic physics of nuclear medicine Nuclear structure Atomic number (Z): the number of protons in a nucleus; defines the position of an element in the periodic table. Mass number (A) is the number of nucleons

More information

Bases of radioisotope diagnostic methods

Bases of radioisotope diagnostic methods Medical, pharmaceutical applications of radioisotopes Bases of radioisotope diagnostic methods Dr. István Voszka Basis of application: radioisotopes have identical behavior in the organism to corresponding

More information

Chapter. Nuclear Chemistry

Chapter. Nuclear Chemistry Chapter Nuclear Chemistry Nuclear Reactions 01 Chapter 22 Slide 2 Chapter 22 Slide 3 Alpha Decay: Loss of an α-particle (a helium nucleus) 4 2 He 238 92 U 234 4 U He 90 + 2 Chapter 22 Slide 4 Beta Decay:

More information

Physics. Medicine. in Nuclear. third edition I

Physics. Medicine. in Nuclear. third edition I SIMON R. CHERRY I PH.D. Professor Department of Biomedical Engineering University of California-Davis Davis, California JAMES A. SORENSON1 PH.D. Emeritus Professor of Medical Physics University of Wisconsin-Madison

More information

Science 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 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 information

Rad T 290 Worksheet 2

Rad T 290 Worksheet 2 Class: Date: Rad T 290 Worksheet 2 1. Projectile electrons travel from a. anode to cathode. c. target to patient. b. cathode to anode. d. inner shell to outer shell. 2. At the target, the projectile electrons

More information

SECTION 8 Part I Typical Questions

SECTION 8 Part I Typical Questions SECTION 8 Part I Typical Questions 1. For a narrow beam of photons, the relaxation length is that thickness of absorber that will result in a reduction of in the initial beam intensity. 1. 1/10. 2. 1/2.

More information

SCINTILLATION DETECTORS & GAMMA SPECTROSCOPY: AN INTRODUCTION

SCINTILLATION DETECTORS & GAMMA SPECTROSCOPY: AN INTRODUCTION SCINTILLATION DETECTORS & GAMMA SPECTROSCOPY: AN INTRODUCTION OBJECTIVE The primary objective of this experiment is to use an NaI(Tl) detector, photomultiplier tube and multichannel analyzer software system

More information

This Week. 3/23/2017 Physics 214 Summer

This Week. 3/23/2017 Physics 214 Summer This Week Atoms and nuclei What are we made of? The periodic table Why does it stop? How were the elements made? Radioactive decay Useful but can be toxic Discovery of X Rays: Cathode Rays and TV sets

More information

List of Nuclear Medicine Radionuclides. Nuclear Medicine Imaging Systems: The Scintillation Camera. Crystal and light guide

List of Nuclear Medicine Radionuclides. Nuclear Medicine Imaging Systems: The Scintillation Camera. Crystal and light guide Nuclear Medicine Imaging Systems: The Scintillation Camera List of Nuclear Medicine Radionuclides Tc99m 140.5 kev 6.03 hours I-131 364, 637 kev 8.06 days I-123 159 kev 13.0 hours I-125 35 kev 60.2 days

More information

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics Nuclear Physics and Astrophysics PHY-30 Dr. E. Rizvi Lecture 4 - Detectors Binding Energy Nuclear mass MN less than sum of nucleon masses Shows nucleus is a bound (lower energy) state for this configuration

More information

Radiation Dose, Biology & Risk

Radiation Dose, Biology & Risk ENGG 167 MEDICAL IMAGING Lecture 2: Sept. 27 Radiation Dosimetry & Risk References: The Essential Physics of Medical Imaging, Bushberg et al, 2 nd ed. Radiation Detection and Measurement, Knoll, 2 nd Ed.

More information

Physics for Radiation Protection

Physics for Radiation Protection James E. Martin Physics for Radiation Protection Third Completely Updated Edition WI LEY WILEY-VCH Verlag GmbH & Co. KGaA I vu Contents Preface XVII 1 Structure of Atoms 1 1.1 Atom Constituents 2 1.2 Structure,

More information

Dosimetry. Sanja Dolanski Babić May, 2018.

Dosimetry. Sanja Dolanski Babić May, 2018. Dosimetry Sanja Dolanski Babić May, 2018. What s the difference between radiation and radioactivity? Radiation - the process of emitting energy as waves or particles, and the radiated energy Radioactivity

More information

Quality Assurance. Purity control. Polycrystalline Ingots

Quality 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 information

Radioisotopes in action. Diagnostic application of radioisotopes. Steps of diagnostic procedure. Information from various medical imaging techniques

Radioisotopes in action. Diagnostic application of radioisotopes. Steps of diagnostic procedure. Information from various medical imaging techniques Radioisotopes in action Diagnostic application of radioisotopes Steps of diagnostic procedure - Radioactive material introduced into the patient - Distribution and alteration of activity is detected -

More information

Radioactivity. The Nobel Prize in Physics 1903 for their work on radioactivity. Henri Becquerel Pierre Curie Marie Curie

Radioactivity. The Nobel Prize in Physics 1903 for their work on radioactivity. Henri Becquerel Pierre Curie Marie Curie Radioactivity Toward the end of the 19 th century, minerals were found that would darken a photographic plate even in the absence of light. This phenomenon is now called radioactivity. Marie and Pierre

More information

CHAPTER 5. Department of Medical Physics, University of the Free State, Bloemfontein, South Africa

CHAPTER 5. Department of Medical Physics, University of the Free State, Bloemfontein, South Africa CHAPTE 5 STATISTICS FO ADIATIO MEASUEMET M.G. LÖTTE Department of Medical Physics, University of the Free State, Bloemfontein, South Africa 5.1. SOUCES OF EO I UCLEA MEDICIE MEASUEMET Measurement errors

More information

Sample Spectroscopy System Hardware

Sample Spectroscopy System Hardware Semiconductor Detectors vs. Scintillator+PMT Detectors Semiconductors are emerging technology - Scint.PMT systems relatively unchanged in 50 years. NaI(Tl) excellent for single-photon, new scintillation

More information

Nuclear Reactions A Z. Radioactivity, Spontaneous Decay: Nuclear Reaction, Induced Process: x + X Y + y + Q Q > 0. Exothermic Endothermic

Nuclear 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 information

MECHANICAL ENGINEERING. Five-year M.Sc. studies School of Mechanical Engineering National Technical University of Athens

MECHANICAL ENGINEERING. Five-year M.Sc. studies School of Mechanical Engineering National Technical University of Athens MECHANICAL ENGINEERING Five-year M.Sc. studies School of Mechanical Engineering National Technical University of Athens Athens, September 8, 2010 Semester 1: Mathematics Ia (52h lectures and exercises)

More information

3. Which of the following statements is (are) TRUE about detector crystals in Anger cameras?

3. Which of the following statements is (are) TRUE about detector crystals in Anger cameras? BioE 1330 - Exam 2 11/13/2018 Answer Sheet - Correct answer is A for all questions 1. Unlike CT, in nuclear medicine A. Bremsstrahlung is not used to produce high-energy photons. B. signal can be increased

More information

City University of Hong Kong

City University of Hong Kong City University of Hong Kong Information on a Course offered by the Department of Physics and Materials Science with effect from Semester A in 2013 / 2014 Part I Course Title: Radiological Physics and

More information

Positron Emission Tomography

Positron Emission Tomography Positron Emission Tomography Presenter: Difei Wang June,2018 Universität Bonn Contents 2 / 24 1 2 3 4 Positron emission Detected events Detectors and configuration Data acquisition Positron emission Positron

More information

Medical Biophysics II. Final exam theoretical questions 2013.

Medical Biophysics II. Final exam theoretical questions 2013. Medical Biophysics II. Final exam theoretical questions 2013. 1. Early atomic models. Rutherford-experiment. Franck-Hertz experiment. Bohr model of atom. 2. Quantum mechanical atomic model. Quantum numbers.

More information

SCINTILLATION DETECTORS AND PM TUBES

SCINTILLATION DETECTORS AND PM TUBES SCINTILLATION DETECTORS AND PM TUBES General Characteristics Introduction Luminescence Light emission without heat generation Scintillation Luminescence by radiation Scintillation detector Radiation detector

More information

Tomography is imaging by sections. 1

Tomography is imaging by sections. 1 Tomography is imaging by sections. 1 It is a technique used in clinical medicine and biomedical research to create images that show how certain tissues are performing their physiological functions. 1 Conversely,

More information

Radiation Detection. 15 th Annual OSC Readiness Training Program.

Radiation Detection. 15 th Annual OSC Readiness Training Program. Radiation Detection 15 th Annual OSC Readiness Training Program www.oscreadiness.org GM Detectors 15 th Annual OSC Readiness Training Program www.oscreadiness.org 1 A closer look 15 th Annual OSC Readiness

More information

Contents. Preface to the First Edition Preface to the Second Edition

Contents. Preface to the First Edition Preface to the Second Edition Contents Preface to the First Edition Preface to the Second Edition Notes xiii xv xvii 1 Basic Concepts 1 1.1 History 1 1.1.1 The Origins of Nuclear Physics 1 1.1.2 The Emergence of Particle Physics: the

More information

Differentiating Chemical Reactions from Nuclear Reactions

Differentiating Chemical Reactions from Nuclear Reactions Differentiating Chemical Reactions from Nuclear Reactions 1 CHEMICAL Occurs when bonds are broken or formed. Atoms remained unchanged, though may be rearranged. Involves valence electrons Small energy

More information

11/10/2014. Chapter 1: Introduction to Medical Imaging. Projection (Transmission) vs. Emission Imaging. Emission Imaging

11/10/2014. Chapter 1: Introduction to Medical Imaging. Projection (Transmission) vs. Emission Imaging. Emission Imaging Chapter 1: Introduction to Medical Imaging Overview of Modalities Properties of an Image: Limitations on Information Content Contrast (both object & image): Brightness difference Sharpness (blur): Smallest

More information

Radiation Protection Training Manual & Study Guide. Jump to the Table of Contents

Radiation Protection Training Manual & Study Guide. Jump to the Table of Contents Radiation Protection Training Manual & Study Guide Jump to the Table of Contents December 1986 Revised 1994 Radiation Safety Office Radiation Protection Training Course Course Outline Time Lecture Topic

More information

Some nuclei are unstable Become stable by ejecting excess energy and often a particle in the process Types of radiation particle - particle

Some nuclei are unstable Become stable by ejecting excess energy and often a particle in the process Types of radiation particle - particle Radioactivity George Starkschall, Ph.D. Lecture Objectives Identify methods for making radioactive isotopes Recognize the various types of radioactive decay Interpret an energy level diagram for radioactive

More information

Module 1. An Introduction to Radiation

Module 1. An Introduction to Radiation Module 1 An Introduction to Radiation General Definition of Radiation Ionizing radiation, for example, X-rays, gamma-rays, α particles Ionizing radiation is capable of removing an electron from the atom

More information

Radioisotopes and PET

Radioisotopes and PET Radioisotopes and PET 1 Radioisotopes Elements are defined by their number of protons, but there is some variation in the number of neutrons. Atoms resulting from this variation are called isotopes. Consider

More information

Nuclear Physics Lab I: Geiger-Müller Counter and Nuclear Counting Statistics

Nuclear Physics Lab I: Geiger-Müller Counter and Nuclear Counting Statistics Nuclear Physics Lab I: Geiger-Müller Counter and Nuclear Counting Statistics PART I Geiger Tube: Optimal Operating Voltage and Resolving Time Objective: To become acquainted with the operation and characteristics

More information

Radioactivity. Lecture 6 Detectors and Instrumentation

Radioactivity. Lecture 6 Detectors and Instrumentation Radioactivity Lecture 6 Detectors and Instrumentation The human organs Neither humans nor animals have an organ for detecting radiation from radioactive decay! We can not hear it, smell it, feel it or

More information

Chapter 21. Preview. Lesson Starter Objectives Mass Defect and Nuclear Stability Nucleons and Nuclear Stability Nuclear Reactions

Chapter 21. Preview. Lesson Starter Objectives Mass Defect and Nuclear Stability Nucleons and Nuclear Stability Nuclear Reactions Preview Lesson Starter Objectives Mass Defect and Nuclear Stability Nucleons and Nuclear Stability Nuclear Reactions Section 1 The Nucleus Lesson Starter Nuclear reactions result in much larger energy

More information

Year 12 Notes Radioactivity 1/5

Year 12 Notes Radioactivity 1/5 Year Notes Radioactivity /5 Radioactivity Stable and Unstable Nuclei Radioactivity is the spontaneous disintegration of certain nuclei, a random process in which particles and/or high-energy photons are

More information

AQA Physics /7408

AQA Physics /7408 AQA Physics - 7407/7408 Module 10: Medical physics You should be able to demonstrate and show your understanding of: 10.1 Physics of the eye 10.1.1 Physics of vision The eye as an optical refracting system,

More information

Figure 1. Decay Scheme for 60Co

Figure 1. Decay Scheme for 60Co Department of Physics The University of Hong Kong PHYS3851 Atomic and Nuclear Physics PHYS3851- Laboratory Manual A. AIMS 1. To learn the coincidence technique to study the gamma decay of 60 Co by using

More information

Mayneord-Phillips Summer School St Edmund Hall, University of Oxford July Proton decays to n, e +, ν

Mayneord-Phillips Summer School St Edmund Hall, University of Oxford July Proton decays to n, e +, ν Positron Emission Tomography Physics & Instrumentation Dimitra G. Darambara, Ph.D Multimodality Molecular Imaging Joint Department of Physics RMH/ICR Outline Introduction PET Physics overview Types of

More information