Gamma Cameras
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Design of Neutron and Gamma Ray Diagnostics for the Start-Up Phase of the DTT Tokamak
46th EPS Conference on Plasma Physics P5.1105 Design of neutron and gamma ray diagnostics for the start-up phase of the DTT tokamak M. Angelone 1, D. Rigamonti 2, M Tardocchi 2, F. Causa 2, S. Fiore 1, L. C. Giacomelli 2, G. Gorini 3,2 , F. Moro 1, M. Nocente 3,2 , M. Osipenko 4, M. Pillon 1, , M. Ripani 4, R. Villari 1 1ENEA, Centro Ricerche Frascati, Frascati, Italy 2Istituto per la Scienza e Tecnologia dei Plasmi, CNR, Milan, Italy 3Dipart. di Fisica “G. Occhialini”, Università degli Studi di Milano-Bicocca, Milano, Italy 4Istituto Nazionale di Fisica Nucleare, Genova, Italy e-mail : [email protected] Abstract The Divertor Tokamak Test (DTT) facility, which is under design for construction in Frascati (Italy), will produce neutron yield up to 1.3*10 17 n/s at full power (H-mode scenario). This calls for an accurate design and selection of the 2.5 MeV neutron diagnostic systems and detectors which can give the comprehensive exploitation of the high neutron fluxes. Measurements of 14 MeV neutrons (which are about 1% of the total neutron yield) coming from the triton burn-up will also be performed. DTT will reach its best performances after a preliminary phase , needed to assess and improve the machine parameters. Here we present the neutron and gamma-ray diagnostics systems which are under design for the initial start-up phase of DTT. The design work benefits from the experience gathered by the community on high power tokamak such as JET. These systems, also called day-1 diagnostics, are: i) Neutron flux monitors which measure the 2.5 and 14 MeV neutron yield s, ii) Neutron/Gamma camera for the reconstruction of the neutron and gamma ray emission profile of the plasma , iii) Hard x-ray monitors for measurements of the bremsstrahlung radiation produced by runway electrons in the 1-40 MeV energy range 1.0 Introduction The Divertor Tokamak Test (DTT) facility, which is under design for construction in Frascati (Italy), will produce neutron yield up to 1.3*10 17 n/s at full power (H-mode scenario). -
Radiation Quick Reference Guide Recommend Contacting Your State Fusion Center
Domestic Nuclear Detection Office If you encounter something suspicious follow your specific local protocols. Radiation Quick Reference Guide Recommend contacting your state fusion center. DNDO is available 24/7 to assist at 1-877-DNDO-JAC / 1-877-363-6522 JAC Information Line 202-254-7179 Email: [email protected] Nuclear Concerns/ Threats 1. Nuclear Weapon - a device that releases nuclear energy in an ex- Isotopes of Concern for use in RDDs - with common uses plosive manner. Uses Highly Enriched Uranium (HEU) and/or 1. Cobalt-60 – cancer treatment, level/ Plutonium. density gauge, teletherapy, radiography, 2. Improvised Nuclear Device (IND) - a nuclear weapon fabricated food sterilization/irradiation, by a terrorist organization or rogue nation. brachytherapy 2. Iridium-192 – Radiography/non- destructive testing, flaw detection, brachy- therapy “cancer seed”, skin cancer Cobalt 60 sources Uranium “superficial” brachytherapy Plutonium 3. Uranium a. Uranium exists naturally in the earth’s crust. Of the different “isotopes” of uranium, U-235 is the one required to produce a Iridium sentinel and nuclear weapon. gamma camera b. Natural uranium contains a small amount of U-235 (<1%) which Cesium Seeds must be separated in complex extraction processes to create HEU. The predominant uranium isotope is U-238. 3. Cesium-137 - Gauge/level gauge, industrial radiography, brachyther- c. Highly Enriched Uranium (HEU) refers to uranium usable in weap- apy/teletherapy, well logging/density gauges ons due to its enrichment in U-235. 4. Strontium-90 – Radioisotope thermoelectric generator (RTG), fis- d. Approximately 25 kg of HEU is required for a nuclear weapon. sion product, industrial gauges, medical treatment e. -
A New Gamma Camera for Positron Emission Tomography
INIS-mf—11552 A new gamma camera for Positron Emission Tomography NL89C0813 P. SCHOTANUS A new gamma camera for Positron Emission Tomography A new gamma camera for Positron Emission Tomography PROEFSCHRIFT TER VERKRIJGING VAN DE GRAAD VAN DOCTOR AAN DE TECHNISCHE UNIVERSITEIT DELFT, OP GEZAG VAN DE RECTOR MAGNIFICUS, PROF.DRS. P.A. SCHENCK, IN HET OPENBAAR TE VERDEDIGEN TEN OVERSTAAN VAN EEN COMMISSIE, AANGEWEZEN DOOR HET COLLEGE VAN DECANEN, OP DINSDAG 20 SEPTEMBER 1988TE 16.00 UUR. DOOR PAUL SCHOTANUS '$ DOCTORANDUS IN DE NATUURKUNDE GEBOREN TE EINDHOVEN Dit proefschrift is goedgekeurd door de promotor Prof.dr. A.H. Wapstra s ••I Sommige boeken schijnen geschreven te zijn.niet opdat men er iets uit zou leren, maar opdat men weten zal, dat de schrijver iets geweten heeft. Goethe Contents page 1 Introduction 1 2 Nuclear diagnostics as a tool in medical science; principles and applications 2.1 The position of nuclear diagnostics in medical science 2 2.2 The detection of radiation in nuclear diagnostics: 5 standard techniques 2.3 Positron emission tomography 7 2.4 Positron emitting isotopes 9 2.5 Examples of radiodiagnostic studies with PET 11 2.6 Comparison of PET with other diagnostic techniques 12 3 Detectors for positron emission tomography 3.1 The absorption d 5H keV annihilation radiation in solids 15 3.2 Scintillators for the detection of annihilation radiation 21 3.3 The detection of scintillation light 23 3.4 Alternative ways to detect annihilation radiation 28 3-5 Determination of the point of annihilation: detector geometry, -
State-Of-The-Art Mobile Radiation Detection Systems for Different Scenarios
sensors Review State-of-the-Art Mobile Radiation Detection Systems for Different Scenarios Luís Marques 1,* , Alberto Vale 2 and Pedro Vaz 3 1 Centro de Investigação da Academia da Força Aérea, Academia da Força Aérea, Instituto Universitário Militar, Granja do Marquês, 2715-021 Pêro Pinheiro, Portugal 2 Instituto de Plasmas e Fusão Nuclear, Instituto Superior Técnico, Universidade de Lisboa, Av. Rovisco Pais 1, 1049-001 Lisboa, Portugal; [email protected] 3 Centro de Ciências e Tecnologias Nucleares, Instituto Superior Técnico, Universidade de Lisboa, Estrada Nacional 10 (km 139.7), 2695-066 Bobadela, Portugal; [email protected] * Correspondence: [email protected] Abstract: In the last decade, the development of more compact and lightweight radiation detection systems led to their application in handheld and small unmanned systems, particularly air-based platforms. Examples of improvements are: the use of silicon photomultiplier-based scintillators, new scintillating crystals, compact dual-mode detectors (gamma/neutron), data fusion, mobile sensor net- works, cooperative detection and search. Gamma cameras and dual-particle cameras are increasingly being used for source location. This study reviews and discusses the research advancements in the field of gamma-ray and neutron measurements using mobile radiation detection systems since the Fukushima nuclear accident. Four scenarios are considered: radiological and nuclear accidents and emergencies; illicit traffic of special nuclear materials and radioactive -
Radiation and Radionuclide Measurements at Radiological and Nuclear Emergencies
Radiation and radionuclide measurements at radiological and nuclear emergencies. Use of instruments and methods intended for clinical radiology and nuclear medicine. Ören, Ünal 2016 Document Version: Publisher's PDF, also known as Version of record Link to publication Citation for published version (APA): Ören, Ü. (2016). Radiation and radionuclide measurements at radiological and nuclear emergencies. Use of instruments and methods intended for clinical radiology and nuclear medicine. Lund University: Faculty of Medicine. Total number of authors: 1 Creative Commons License: Other General rights Unless other specific re-use rights are stated the following general rights apply: Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. • Users may download and print one copy of any publication from the public portal for the purpose of private study or research. • You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal Read more about Creative commons licenses: https://creativecommons.org/licenses/ Take down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. LUND UNIVERSITY PO Box 117 221 00 Lund +46 46-222 00 00 Download date: 24. Sep. 2021 Radiation and radionuclide measurements at radiological and nuclear emergencies Use of instruments and methods intended for clinical radiology and nuclear medicine Ünal Ören DOCTORAL DISSERTATION by due permission of the Faculty of Medicine, Lund University, Sweden. -
Positron Emission Tomography
Positron emission tomography A.M.J. Paans Department of Nuclear Medicine & Molecular Imaging, University Medical Center Groningen, The Netherlands Abstract Positron Emission Tomography (PET) is a method for measuring biochemical and physiological processes in vivo in a quantitative way by using radiopharmaceuticals labelled with positron emitting radionuclides such as 11C, 13N, 15O and 18F and by measuring the annihilation radiation using a coincidence technique. This includes also the measurement of the pharmacokinetics of labelled drugs and the measurement of the effects of drugs on metabolism. Also deviations of normal metabolism can be measured and insight into biological processes responsible for diseases can be obtained. At present the combined PET/CT scanner is the most frequently used scanner for whole-body scanning in the field of oncology. 1 Introduction The idea of in vivo measurement of biological and/or biochemical processes was already envisaged in the 1930s when the first artificially produced radionuclides of the biological important elements carbon, nitrogen and oxygen, which decay under emission of externally detectable radiation, were discovered with help of the then recently developed cyclotron. These radionuclides decay by pure positron emission and the annihilation of positron and electron results in two 511 keV γ-quanta under a relative angle of 180o which are measured in coincidence. This idea of Positron Emission Tomography (PET) could only be realized when the inorganic scintillation detectors for the detection of γ-radiation, the electronics for coincidence measurements, and the computer capacity for data acquisition and image reconstruction became available. For this reason the technical development of PET as a functional in vivo imaging discipline started approximately 30 years ago. -
ITER Relevant Runaway Electron Studies in the FTU Tokamak
ITER Relevant Runaway Electron Studies in the FTU Tokamak by Zanaˇ Popovi´c A dissertation submitted in partial fulfilment of the requirements for the degree of Doctor of Philosophy in Plasmas y Fusi´on Nuclear Universidad Carlos III de Madrid Directors: Prof Dr Jos´eRam´on Mart´ın Sol´ıs Dr Basilio Esposito Tutor: Prof Dr Jos´eRam´on Mart´ın Sol´ıs July 2019 Esta tesis se distribuye bajo licencia “Creative Commons Reconocimiento – No Comercial – Sin Obra Derivada” ii Dedication To my family, VVBM iii iv Acknowledgements I would like to thank an exceptional man, my thesis director and supervisor Prof Jos´eRam´on Mart´ın Sol´ıs. I have been lucky to be his student and am very grateful for all the help and caring guidance he has given me, for his patience and organisation throughout this work, especially during one of the most challenging years I have had. I appreciate immensely his expertise and dedication to teaching, which made this thesis possible. I would also like to thank my thesis co-director, Dr Basilio Esposito, for the invaluable mentoring and direction over the years, and for the delightful hospitality he and his family provided during my research visits in Frascati. Many thanks to the people I collaborated with as a part of the FTU team at ENEA Research Centre, especially Drs Daniele Carnevale, Daniele Marocco, Federica Causa and Mateusz Gospodarczyk, as well as the other members of the FTU team and supporting staff for creating a stimulating and cheerful work environment during long experiments. This journey was filled with interesting times spent with the people from the Department of Physics at Universidad Carlos III de Madrid. -
Medical Nuclear Physics Performance Monitoring of Gamma Cameras
The American College of Radiology, with more than 30,000 members, is the principal organization of radiologists, radiation oncologists, and clinical medical physicists in the United States. The College is a nonprofit professional society whose primary purposes are to advance the science of radiology, improve radiologic services to the patient, study the socioeconomic aspects of the practice of radiology, and encourage continuing education for radiologists, radiation oncologists, medical physicists, and persons practicing in allied professional fields. The American College of Radiology will periodically define new practice parameters and technical standards for radiologic practice to help advance the science of radiology and to improve the quality of service to patients throughout the United States. Existing practice parameters and technical standards will be reviewed for revision or renewal, as appropriate, on their fifth anniversary or sooner, if indicated. Each practice parameter and technical standard, representing a policy statement by the College, has undergone a thorough consensus process in which it has been subjected to extensive review and approval. The practice parameters and technical standards recognize that the safe and effective use of diagnostic and therapeutic radiology requires specific training, skills, and techniques, as described in each document. Reproduction or modification of the published practice parameter and technical standard by those entities not providing these services is not authorized. 2018 (CSC/BOC)* ACR–AAPM TECHNICAL STANDARD FOR NUCLEAR MEDICAL PHYSICS PERFORMANCE MONITORING OF GAMMA CAMERAS PREAMBLE This document is an educational tool designed to assist practitioners in providing appropriate radiologic care for patients. Practice Parameters and Technical Standards are not inflexible rules or requirements of practice and are not intended, nor should they be used, to establish a legal standard of care1. -
(EANM) Acceptance Testing for Nuclear Medicine Instrumentation
Eur J Nucl Med Mol Imaging (2010) 37:672–681 DOI 10.1007/s00259-009-1348-x GUIDELINES Acceptance testing for nuclear medicine instrumentation Ellinor Busemann Sokole & Anna Płachcínska & Alan Britten & on behalf of the EANM Physics Committee Published online: 5 February 2010 # EANM 2010 Keywords Quality control . Quality assurance . requirement that acceptance testing be performed should Acceptance testing . Nuclear medicine instrumentation . be included in the purchase agreement of an instrument. Gamma camera . SPECT. PET. CT. Radionuclide calibrator. This agreement should specify responsibilities regarding Thyropid uptake probe . Nonimaging intraoperative probe . who does acceptance testing, the procedure to be followed Gamma counting system . Radiation monitors . when unsatisfactory results are obtained, and who supplies Preclinical PET the required phantoms and software. A specific time slot must be allocated for performing acceptance tests. Introduction Acceptance and reference tests These recommendations cover acceptance and reference tests that should be performed for acceptance testing of Acceptance tests are performed to verify that the instrument instrumentation used within a nuclear medicine department. performs according to its specifications. Each instrument is These tests must be performed after installation and before supplied with a set of basic specifications. These have been the instrument is put into clinical use, and before final produced by the manufacturer according to standard test payment for the device. These recommendations -
PET Imaging: an Overview and Instrumentation
CONTINUING EDUCATION PET Imaging: An Overview and Instrumentation Farhad Daghighian, Ronald Sumida, and Michael E. Phelps Division ofNuclear Medicine and Biophysics, Department ofRadiological Sciences; and Laboratory ofNuclear Medicine, Laboratories of Biomedical and Environmental Sciences (DOE)*, UCLA School ofMedicine, Los Angeles, California gen in many chemical compounds. None of the above This is the first article of a four-part series on positron elements have any isotope which emits a gamma ray emission tomography (PET). Upon completing the article, the suitable for imaging with a gamma camera. Hence, one reader should be able to: (1) comprehend the basic principles of the advantages of PET over SPECT is that it deals ofPET; (2) explain various technical aspects; and ( 3) identify with isotopes of those elements that are the building radiopharmaceuticals used in PET imaging. blocks of biomolecules. BRIEF HISTORY Positron emission tomography (PET) is a rapidly growing AND FUTURE OUTLOOK OF PET technique within nuclear medicine. A radiopharmaceutical Positron imaging began with the two-dimensional sodium labeled with a positron emitting isotope is administered intra iodide detector-based scanning devices developed in the late venously or by inhalation to the patient, and the PET scanner 1950s and 1960s by Wrenn et al. ( 4) and Brownell et al. (5). images the distribution of that radiopharmaceutical. It is the Burham and Brownell also developed a dual-headed multi only imaging modality capable of providing quantitative in detector camera that provided a limited form of"focal plane" formation about biochemical and physiologic processes (J- tomography ( 6). Robertson and Niel took a different ap 3). Other techniques like magnetic resonance imaging (MRI) proach and used a "blurring tomography" with a circular and x-ray computerized tomography (CT) generally image array of sodium iodide detectors ( 7). -
Time for a Next-Generation Nuclear Medicine Gamma Camera?
Time for a Next-Generation Nuclear Medicine Gamma Camera? I. George Zubal, PhD, Program Director for Nuclear Medicine, CT, and X-Ray, National Institute of Biomedical NEWSLINE Imaging and Bioengineering, Bethesda, MD al Anger invented the gamma camera in 1957, and it Imaging of these radiotherapy ligands has been in- is fair to say that the basic geometry and components vestigated. Two of the 6 photopeaks (113 and 208 keV) of H 177 of his camera design have remained substantially the Lu were imaged with additional energy windows set to same, while its use in general clinical applications has been subtract scatter from higher energy emissions (1). An array optimized for imaging 140-keV gamma rays. The past 60 of bremsstrahlung emissions, together with internal pair- years have seen some improvements in NaI scintillators, production annihilation radiation, was used to produce readout electronics, collimators, reconstruction algorithms, 90Y images (2). Images of 223Ra (and its daughter 219Rn) and image analysis. During a short period in the late 1990s were acquired using 3 photopeaks (85, 154, and 270 keV) and early 2000s, opposing Anger cameras were used for with 3 additional windows to deal with scattered events (3). clinically acquiring positron-emitting isotopes, and some Imaging protocols become more complicated for other a camera components were reengineered for imaging 511- emitters, including 225Ac, 211At, 212Pb, and others yet to be keV coincident photons. Not surprisingly, dedicated PET considered for therapy. These isotopes pose a challenge to cameras proved to be the better choice for imaging PET nuclear medicine camera systems because the radiations lie radiotracers. -
Instrumentation
INSTRUMENTATION Our Department currently consists of: Philips Gemini-GXL 6 slice PET/CT scanner. GE Discovery 710 - 128slice Time of Flight (TOF) PET/CT scanner 3 SPECT cameras: o 2-GE Discovery(SPECT/CT) o Philips Skylight. GE Lunar Prodigy Bone Mineral Densitometer. GE Centricity PACS/RIS. To learn about our imaging instrumentation, browse through the following Internet web sites: www.philips.com/healthcare www.gehealthcare.com WHAT IS A SPECT CAMERA? A SPECT camera is an imaging device which detects the gamma radiation being emitted from patients after administration of a radiopharmaceutical. It is based on the Anger camera, named after Hal Anger who developed the first gamma camera in the 1950’s. A SPECT camera consists of one or more heads mounted onto a gantry, with an imaging bed or table. The head is comprised of flat crystal detectors coupled to photomultiplier tubes. When a gamma ray is detected by the crystal it makes the crystal glow, and the photomultiplier tubes convert this light glow into an electrical signal. These electrical signals are recorded by a computer which then displays a 2D image on the monitor which reflects the distribution and relative concentration of the radiopharmaceutical within the patient’s body. Depending on the scan type and the diagnosis in question, the patient may have images performed as soon as the radiopharmaceutical is administered (dynamic imaging) or images may be acquired after a specific time delay. The SPECT camera can be used for stationary (static) imaging or may move in one motion along the body’s contour (whole body sweep).