APPLIED GAMMA-RAY<br />
SPECTROMETRY<br />
BY<br />
<br />
C. E. CROUTHAMEL<br />
Argonne National Laboratory, U.S.A.<br />
<br />
SECOND E D I T I O N<br />
COMPLETELY REVISED AND E N L A R G E D<br />
BY<br />
<br />
F. ADAMS AND R. DAMS<br />
Institute of Nuclear Sciences,<br />
Ghent State University,<br />
Belgium<br />
<br />
P E R G A M O N PRESS<br />
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Copyright (C) 1970 F. Adams and R. Dams<br />
All Rights Reserved. No part of this publication may he<br />
reproduced, stored in a retrieval system, or transmitted, in<br />
any form or by any means, electronic, mechanical,<br />
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permission of Pergamon Press Ltd.<br />
First edition 1960<br />
Second revised and enlarged edition 1970<br />
Reprinted 1975<br />
Library of Congress Catalog Card No. 79-114847<br />
<br />
Printed in Great Britain by<br />
Biddies Ltd., Guildford, Surrey<br />
ISBN 0 08 006888 X<br />
<br />
PREFACE TO THE SECOND EDITION<br />
10 years have passed since the first edition of this book. Much progress has been<br />
made during the past decade, especially in high resolution gamma-ray spectrometry using<br />
semiconductor detectors. The increasing efficiency and the improving energy resolution<br />
made the scientists realize that they had at hand a new and beautiful research tool. Im<br />
proved amplifying and analyzing equipment were necessary to realize the full abilities of<br />
high resolution detectors.<br />
Like the previous edition, the new one is primarily meant for experimentalists. Chapter 1<br />
contains the various decay processes and the possible interaction mechanisms of gamma<br />
radiation with matter. Chapters 2, 3 and 4 deal with properties and fabrication of respec<br />
tively scintillation detectors, semiconductor detectors, and proportional gas counters.<br />
Chapter 5 includes the description of basic equipment, i.e. amplifiers, analyzers, special<br />
spectrometer arrangements, and detector shielding. Energy and time resolution is treated<br />
in Chapter 6, whereas Chapter 7 deals with quantitative calibration. The quantitative and<br />
qualitative interpretation of the spectra is treated in Chapter 8. The last chapter describes<br />
the analytical applications of gamma-ray and X-ray spectrometry in tracer studies, activa<br />
tion analysis, fission product studies, and X-ray fluorescence analysis. Chapters 3, 5 and<br />
8 are entirely new, while the other chapters were extended and brought up to date.<br />
Appendix II is extended with the gamma-ray spectra of 46, mainly short-lived or neutron<br />
deficient, isotopes. Appendix III contains about 220 gamma-ray spectra taken with a lithium<br />
drifted germanium detector. The calculated intrinsic efficiencies for sodium iodide crystals<br />
are provided in Appendix IV, while a short compilation of internal conversion coefficients<br />
is given in Appendix V. The tabulations of the characteristic X-ray energies (Appendix I)<br />
and of the nuclear data by photon energy and half-life sequences (Appendix VI) have been<br />
supplemented by a sequence of precisely determined photon energies (Appendix VII).<br />
We are deeply indebted to Professor Dr. J. Hoste, Director of the Institute for Nuclear<br />
Sciences, Radio- and Analytical Chemistry Division, for his whole-hearted support and<br />
valuable advice and suggestions. We gratefully acknowledge the help of Dr. A. Speecke for<br />
reading portions of the manuscript and offering many valuable suggestions. During the<br />
preparation of the manuscript we have enjoyed many discussions with friends and colleagues.<br />
We should like to thank, particularly, P. de Regge, J. P. Francois, J. Fuger, J. I. Kim, and R.<br />
Van Inbroukx for providing us with a number of pure gamma sources. For the preparation of<br />
Appendices II, III, and VII, numerous irradiations were performed with the Thetis reactor<br />
and with the linear electron accelerator, both at the Institute of Nuclear Sciences, Ghent.<br />
We are grateful to all those in charge of the exploitation of these machines and especially<br />
to Dr. A. Speecke and Ir. K. Kiesel. We are grateful to Miss M. Helsen and Mrs. J. GorleeZels for preparing the numerous drawings and for their unfailing help in the preparation of<br />
the manuscript.<br />
We thank those who allowed us to use data from their work. We made every endeavor<br />
to acknowledge this help in the text.<br />
<br />
NEARLY<br />
<br />
Ghent, Belgium<br />
<br />
F.<br />
xi<br />
<br />
ADAMS,<br />
<br />
R.<br />
<br />
DAMS<br />
<br />
PREFACE TO THE FIRST EDITION<br />
book is the outgrowth of the rapidly increasing and widespread application of gammaray spectrometry to many fields other than nuclear physics. Chemists, biologists, engineers,<br />
and other research workers applying this valuable tool will face the task of interpreting<br />
the gamma-ray spectra. Each radioactive nuclide and detector combination will present a<br />
virtually unique situation with regard to scattering, energy resolution, and relative inten<br />
sities in the various energy regions of the spectrum. The accurate qualitative interpretation<br />
of a gamma-ray spectrum requires a careful evaluation of the source and intensity of the<br />
various peaks which may be generated in the spectrum for a given experimental situation.<br />
The discussion in Chapters 1 and 2 deal with the intrinsic and extrinsic variables which<br />
affect the observed gamma-ray and X-ray spectra. Most of the effects of these variables are<br />
illustrated in Appendix II. Appendices I and IV are tabulations of the characteristic X-ray<br />
energies in keV and of the nuclear data by photon energy and half-life sequences. These<br />
data are designed to aid in the rapid qualitative interpretation of the gamma-ray spectra.<br />
The quantitative calibration of the spectra is treated in Chapter 3 with supplementary<br />
data in Appendix III.<br />
Finally, some of the most widely utilized applications are discussed in Chapter 4, with<br />
particular emphasis given to activation analysis.<br />
The authors are indebted to many colleagues at the Argonne National Laboratory for<br />
support and assistance in preparing the manuscript, in particular, Richard C. Vogel and<br />
Victor H. Munnecke for their continued support and valuable suggestions in examining<br />
the manuscript, also to Peter Kafalas, Ellis P. Steinberg, Donald Engelkemeir, Harold A.<br />
May and Charles E. Miller for reading portions of the manuscript and offering valuable<br />
criticisms. Willard H. McCorkle and Joseph I. McMilien have given invaluable assistance<br />
with the many irradiations at CP-5. The authors are also indebted to Dorothy A. Carlson<br />
and her co-workers in the Graphic Arts Department for preparing the numerous drawings;<br />
Gene H. McCloud, Allen A. Madson, and Marion Crouthamel for their many hours of<br />
assistance in the checking and preparation of the manuscript.<br />
THIS<br />
<br />
Lemont, Illinois<br />
C. E. CROUTHAMEL<br />
<br />
INTRODUCTION<br />
SCINTILLATION counting, one of the oldest radiation detection techniques, has gone through<br />
several developmental phases. The visually detected scintillations of energetic alpha parti<br />
cles absorbed in thin films of zinc sulfide crystals were first noted by Sir William Crookes<br />
and also independently by Elster and Geitel in 1903. Crookes and Regener had developed<br />
an early apparatus, the spinthariscope and its' associated counting techniques, by 1908.<br />
The spinthariscope was made up of a microscope of magnification about thirty with an<br />
objective of large numerical aperture, a zinc sulfide copper-activated screen, a source of<br />
alpha particles, and a gas-tight box which could be evacuated and in which these compo<br />
nents as well as scatterers and absorbers could be mounted. In the 25 years following its<br />
development the spinthariscope produced many valuable contributions to the field of nuclear<br />
research. Its application made possible detailed studies of the scattering of alpha particles<br />
by thin foils and thus first indicated the presence, and then the size and charge, of the atomic<br />
nucleus. Also, the first evidence of artificial disintegration of stable isotopes was obtained<br />
by Rutherford with this instrument in 1919. Anyone familiar with present-day instrumenta<br />
tion will appreciate the high quality of the data gathered by means of this early instrument.<br />
An account and analysis of the numerous pioneering experiments which employed the<br />
spinthariscope is given by Rutherford et α/.(1)<br />
The visual scintillation counter became obsolete in the 1930's, and the next 20 years<br />
were characterized by the rapid growth and development of electronic counting techniques.<br />
Gas-filled ionization chambers in which the incident charged particles generate ion pairs<br />
were used as the basic detector. With these gas-filled systems there are three well-defined<br />
operating »methods—the ionization detector, the proportional counter, and the GeigerMüller counter.<br />
In the first method the ionization chamber consists of two electrodes in a gas medium.<br />
When the chamber is placed in a radiation field the gas is ionized. If a steady voltage is<br />
also applied to the electrodes, the ion pairs separate under the influence of the electric field<br />
and current will flow in an external circuit connected to the ionization chamber. As the<br />
chamber voltage is increased, this current quickly reaches a limiting value which is pro<br />
portional to the rate of production of the ion pairs. In order to measure this saturation<br />
current, however, it is necessary to use extremely sensitive current measuring devices.<br />
Probably the most reliable and sensitive current measuring device applied to ionization<br />
chambers is the vibrating reed electrometer.<br />
The second operating method of the gas-filled systems, the proportional counter, uses a<br />
cylindrical or spherical chamber with a positive electric field originating on a thin wire<br />
electrode. Multiplication of the signal occurs in the vicinity of the wire where the electric<br />
field intensity is great enough to cause the incoming primary electrons to produce miniature<br />
avalanches öf electrons. The gas multiplication is limited so that the final pulse produced is<br />
proportional to the number of primary electrons generated along the track of the incident<br />
ionizing particle. The proportional counter requires carefully designed amplifiers and very<br />
stable, noise-free high voltage and power supplies. This counter is now generally accepted<br />
for alpha and beta counting as one of the most useful and widely applied systems in the<br />
XV<br />
<br />