Saha | Physics and Radiobiology of Nuclear Medicine | E-Book | sack.de
E-Book

E-Book, Englisch, 320 Seiten, eBook

Saha Physics and Radiobiology of Nuclear Medicine

E-Book, Englisch, 320 Seiten, eBook

ISBN: 978-0-387-36281-6
Verlag: Springer US
Format: PDF
Kopierschutz: 1 - PDF Watermark



A new edition of a book is always warranted when it needs to be updated because of advances in the ?eld over time. Although the basics of physics, instrumentation, and radiobiology have not changed, their tech- logical applications have been changing and improving continually. Nuclear medicine professionals worldwide appreciate the book so much that the previous edition has been published in Japanese. Changes in content and appreciation of the book are the two guiding factors in writing this third edition. Like the previous editions, the book is aimed at residents taking the American Board of Nuclear Medicine, the American Board of Radiology (Physics part), and the American Board of Radiology with Special C- petency in Nuclear Medicine examinations,and for the technologists taking the Nuclear Medicine Technology Certifying Board. The book contains 16 chapters,and at the end of each chapter,references and suggested readings have been updated and new questions have been added where appropriate. The ?rst 10 chapters have only minor changes because of the basic nature of the contents. A section on the chi-square test and evaluation of diagnostic tests has been added in Chapter 4. Additional radionuclides have been included in Table 5. 1. In Chapter 8, the section on scintillation detectors has been rearranged and the section on dead time has been expanded. In Chapter 10, the sections on uniformity, gamma camera tuning, and quality control tests have been revised. A new section on software and DICOM has been added in Chapter 11.
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Weitere Infos & Material


Structure of Matter.- Radioactive Decay.- Kinetics of Radioactive Decay.- Statistics of Radiation Counting.- Production of Radionuclides.- Interaction of Radiation with Matter.- Gas-Filled Detectors.- Scintillation and Semiconductor Detectors.- Gamma Cameras.- Performance Parameters of Gamma Cameras.- Digital Computers in Nuclear Medicine.- Single Photon Emission Computed Tomography.- Positron Emission Tomography.- Internal Radiation Dosimetry.- Radiation Biology.- Radiation Regulations and Protection.


"6 Interaction of Radiation with Matter (p. 56)

All particulate and electromagnetic radiations can interact with the atoms of an absorber during their passage through it, producing ionization and excitation of the absorber atoms. These radiations are called ionizing radiations. Because particulate radiations have mass and electromagnetic radiations do not, the latter travel through matter longer distance before losing all energy than the former of the same energy. Electromagnetic radiations are therefore called penetrating radiations and particulate radiations nonpenetrating radiations.The mechanisms of interaction with matter, however, differ for the two types of radiation, and therefore they are discussed separately.

Interaction of Charged Particles with Matter

The energetic charged particles such as a-particles, protons, deuterons, and b-particles (electrons) interact with the absorber atoms, while passing through it.The interaction occurs primarily with the orbital electrons of the atoms and rarely with the nucleus. During the interaction, both ionization and excitation as well as the breakdown of the molecule may occur. In excitation, the charged particle transfers all or part of its energy to the orbital electrons, raising them to higher energy shells. In ionization, the energy transfer may be suf?cient to overcome the binding energy of the orbital electrons, ultimately ejecting them from the atom.

Electrons ejected from the atoms by the incident charged particles are called primary electrons, which may have suf?cient kinetic energy to produce further excitation or ionization in the absorber. The high-energy secondary electrons from secondary ionizations are referred to as delta (d-) rays. The process of excitation and ionization will continue until the incident particle and all electrons come to rest. Both these processes may rupture chemical bonds in the molecules of the absorber, forming various chemical entities. In ionization, an average energy of W is required to produce an ion pair in the absorber and varies somewhat with the type of absorber.

The value of W is about 35 eV in air and less in oxygen and xenon gases but falls in the range of 25–45 eV for most gases. The process of ionization, that is, the formation of ion pairs, is often used as a means of the detection of charged particles in ion chambers and Geiger–Müller counters described in Chapter 7. Three important quantities associated with the passage of charged particles through matter are speci?c ionization, linear energy transfer, and range of the particle in the absorber, and these are described next."


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