All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted, in any form or by any means, electronic, mechanical, photocopying, recording or otherwise, except as permitted by law. Advice on how to obtain permission to reuse material from this title is available at http://www.wiley.com/go/ permissions.
The right of Stephen W.S. McKeever to be identified as the author of this work has been asserted in accordance with law.
Registered Offices
John Wiley & Sons Ltd, The Atrium, Southern Gate, Chichester, West Sussex, PO19 8SQ, UK
John Wiley & Sons, Inc., 111 River Street, Hoboken, NJ 07030, USA
Editorial Office
John Wiley & Sons Ltd, The Atrium, Southern Gate, Chichester, West Sussex, PO19 8SQ, UK
For details of our global editorial offices, customer services, and more information about Wiley products visit us at www.wiley.com.
Wiley also publishes its books in a variety of electronic formats and by print-on-demand. Some content that appears in standard print versions of this book may not be available in other formats.
Limit of Liability/Disclaimer of Warranty
In view of ongoing research, equipment modifications, changes in governmental regulations, and the constant flow of information relating to the use of experimental reagents, equipment, and devices, the reader is urged to review and evaluate the information provided in the package insert or instructions for each chemical, piece of equipment, reagent, or device for, among other things, any changes in the instructions or indication of usage and for added warnings and precautions. While the publisher and authors have used their best efforts in preparing this work, they make no representations or warranties with respect to the accuracy or completeness of the contents of this work and specifically disclaim all warranties, including without limitation any implied warranties of merchantability or fitness for a particular purpose. No warranty may be created or extended by sales representatives, written sales materials or promotional statements for this work. The fact that an organization, website, or product is referred to in this work as a citation and/or potential source of further information does not mean that the publisher and authors endorse the information or services the organization, website, or product may provide or recommendations it may make. This work is sold with the understanding that the publisher is not engaged in rendering professional services. The advice and strategies contained herein may not be suitable for your situation. You should consult with a specialist where appropriate. Further, readers should be aware that websites listed in this work may have changed or disappeared between when this work was written and when it is read. Neither the publisher nor authors shall be liable for any loss of profit or any other commercial damages, including but not limited to special, incidental, consequential, or other damages.
Library of Congress Cataloging-in-Publication Data
Names: McKeever, S. W. S., 1950 - author.
Title: A course in luminescence measurements and analyses for radiation dosimetry / by Stephen W. McKeever.
Description: Chichester, John Wiley & Sons, 2022. | Includes bibliographical references and index.
Identifiers: LCCN 2022000515 (print) | LCCN 2022000516 (ebook) | ISBN 9781119646891 (hardback) | ISBN 9781119646914 (pdf) | ISBN 9781119646921 (epub)
LC record available at https://lccn.loc.gov/2022000515
LC ebook record available at https://lccn.loc.gov/2022000516
Cover image: Courtesy of Stephen W.S.McKeever
Cover design by Wiley
Set in 10/12pt and TimesLTStd by Integra software private Ltd, Puducherry, India.
To Claire, Declan, James and Lydia
3.2
3.3
3.5
3.6
3.6.1
3.6.2
3.7.3
3.8.1
3.7.1.3
3.8.2
3.7.3.4
3.8.1.1
3.8.1.2
3.8.1.3
3.8.1.4
3.8.1.5
3.8.2.1
3.8.2.2
3.8.2.3
4.3
4.3.3.3
5.1
5.2
5.2.1
5.2.1.1
5.3
5.2.3
5.2.4
5.2.5
5.2.5.1
5.2.5.2
5.2.5.3
5.2.5.4
5.2.7.1
5.2.7.3
5.2.8
5.3.1
5.3.2
5.3.3
5.3.1.1
5.3.3.1
5.3.3.2
5.3.4
5.3.4.1
5.3.4.2
5.3.5
5.3.6
5.3.7
5.3.8
5.3.9
5.3.10
6
6.2.1
6.2.2
6.2.3
6.2.4
6.2.1.1
6.2.2.1
6.2.2.2
6.2.6
6.2.7
6.2.5.1
6.2.6.1
6.2.6.2
6.2.7.1
7.2.2
7.2.1.4
7.2.1.5
7.2.1.6
7.2.1.8
7.2.2.1
7.2.2.2
7.2.2.3
7.2.2.4
7.2.2.5
7.2.2.6
7.2.2.7
7.2.3
8.2.1
8.2.1.2
8.2.1.3
8.2.1.4
8.2.1.5
8.2.1.6
8.2.2
9
9.2.1.2
9.2.1.3 Buildup Curves:
9.2.1.4
9.2.2
Preface
The detection of ionizing radiation using luminescence methods has been at the forefront of radiation research ever since the earliest discoveries of radiation, radioactivity, and the structure of the atom. The list of pioneering names in the discovery of radiation is lengthy and impressive – Wilhelm Roentgen, Edmond and Henri Becquerel, Ernest Rutherford, Marie Curie, James Chadwick, and numerous others. Many of these pioneers used luminescence of one type or form in their studies, including (using the modern names) phosphorescence, thermoluminescence, and optically stimulated luminescence. Today’s researchers use these techniques and others related to them in a wide range of radiation detection and measurement applications, including personal, environmental, medical, and space dosimetry, and embrace both very low as well as very high radiation dose regimes.
The genesis of this book is a course, given by the author, to graduate students at Oklahoma State University. The intended readers are graduate students (and undergraduate students who are performing research in these areas), and other beginning researchers in this field of study (e.g., postdoctoral fellows and new researchers entering the field). More experienced researchers may also find the book helpful to refresh their conceptual understanding of the topics. The benefit to the reader will be to see how the techniques relate in a holistic manner and to see how the fundamental processes that describe the phenomena can be used to explain many different experimental characteristics.
To new researchers entering the field, the array of measurement and data analysis techniques can be bewildering. Experimental collection of the data may seem simple on first introduction, but useful and reliable analysis requires attention to small details and knowledge of fundamental principles, along with very careful experimental technique. A phrase I often used with my students was that they will spend most of their time learning how to do the experiment properly before they have a reliable data set for analysis. And then what of that analysis? How should they interpret the results that they obtain? What is the best analytical approach, and why?
What this book is: This book presents a course of instruction for beginning students, or for more-experienced researchers new to the field, into three of the main and currently used luminescence phenomena in radiation dosimetry, namely, thermoluminescence (TL), optically stimulated luminescence (OSL), and radiophotoluminescence (RPL). The book outlines the theoretical background of each technique and stresses the connections between them. In doing so, the book treats luminescence techniques for radiation dosimetry holistically, beginning with the basic concepts and showing how the three techniques are related within the processes of energy storage, charge transfer, and defect interactions.
The book emphasizes pedagogy rather than the latest research. State-of-the-art research is included only if it demonstrates a principle or opens new insight into physical mechanisms. Thus, the primary purpose of the book is to teach beginning researchers in the field about the three techniques, their similarities and distinctions, and their applications. The intent is to
provide the reader with the building blocks with which they can examine the latest research and have a sufficient understanding of it to enable them to raise questions and conceive future research programs to answer those questions.
A note on the Exercises: To emphasize the book as a teaching tool, several substantial Exercises are introduced at various points in the book for the reader to test their understanding of the subject matter being discussed. These include derivations of important relationships, or numerical simulations, or solutions to differential equations, etc., in order to demonstrate the various processes. Some are prescriptive, but others are open ended, requiring the reader to draw their own conclusions from the results of the Exercises. The Exercises also include analysis of real experimental data. For this purpose, the book has a companion website where the reader will find some original data sets (TL, OSL, RPL) that may be used by the reader to analyse using the material learned from the book. New data and new problems may be introduced via the web site in the future and in this way the book will be updated and refreshed for future students. In this sense, the author hopes that the book will serve as a “living” teaching tool.
Although it is recommended that the Exercises be worked one by one in the order given, the reader may wish to skip some of the Exercises if they do not align strongly with the reader’s own research interests. Many of them are lengthy. While most are designed for the individual reader, supervisors and advisors may decide that some may be better solved as group exercises, perhaps as part of a tutorial. Some may even form the basis of internal research projects and reports.
What this book is not: Firstly, the book is not a course in radiation dosimetry. That topic is adequately covered in many excellent existing textbooks.
Secondly, the book is not an updated summary of the latest research on luminescence dosimetry. It is not a review. Several books exist on the topics of TL, OSL, and (to a much lesser extent) RPL. Each, by and large, is a summary of the latest research and newest developments and applications of the techniques (at the times that the books were written) and generally deal with the chosen topic (i.e. TL, OSL, or RPL) in isolation. For example, several texts exist on TL and related thermally stimulated processes, introducing the standard energy band diagrams and kinetic equations, analysis of TL glow curves, and subsequent applications. One can also identify similar texts on OSL. (Only one text, of which this author is aware, deals with RPL.) Rarely, however, do the published books relate one technique to another, except in passing. This is especially true of RPL and its relationship to TL and/or OSL.
Nor does the book present a list of references to all the latest research or pivotal developments. The original material is for the reader to find in independent study. Only when the author has judged that additional reading would be useful, or that the meaning requires more explanation, are references to the original literature included. Readers who wish to avail themselves of the latest research are advised to refer to the proceedings of relevant conferences in the field and to original, peer-reviewed literature. The author hopes that this book will assist in an understanding of the material readers find in those publications.
To achieve the goals outlined above, the book is constructed in two parts. Part I deals with theory, models, and kinetics. It can be considered as a “tool-box” into which the reader can delve to help form an understanding of the underlying principles which govern luminescence phenomena. In the same way that a designer of a new aircraft or of a sophisticated automobile will need an understanding of the basic principles of mechanics, materials, and aerodynamics, so too should the budding researcher into luminescence dosimetry have at hand a similar understanding of the basics of electronic processes in solids, particularly the kinetics of charge generation and storage, stimulation, and recombination. Armed with this “tool-box” the reader can more fully appreciate the experimental phenomena described in Part II.
Part II discusses several real examples of the fundamentals outlined in Part I. The intent is to illustrate how the principles developed in Part I have been used in experiments to measure, understand, and exploit the properties of luminescence materials, especially as they relate to radiation dosimetry. To learn from the wisdom of Albert Einstein, knowing the luminescence properties of a material is one thing, but real progress is made only when we understand them. The author’s hope is that the reader can use the items in the “tool-box” and apply them to the properties of real materials in order to gain that understanding, and perhaps lead to greater creativity and innovation. As a caveat, however, the reader may be wise to recall the words of Prussian Field Marshal Helmuth von Moltke, which the author paraphrases as few theories survive first contact with an experiment.
Acknowledgments
The author gratefully acknowledges the assistance of many colleagues in reading certain chapters and sections of the text, correcting mistakes, and making very positive suggestions. Also acknowledged are those who provided example data sets for use on the accompanying web site for reader analysis. Specific thanks go to Adrie Bos, Mayank Jain, Vasilis Pagonis, Nigel Poolton, Peter Townsend, Sergey Sholom, and Eduardo Yukihara, for their unfailing assistance in reading parts of the text and providing vital feedback to the author. Any remaining errors are the author’s own. Special thanks, however, go to my friend and long-time colleague, Sergey Sholom, for not only reading multiple sections of the book, but also in answering my persistent calls for original data for inclusion in the book and for uploading to the web site for use in the Exercises and for analysis by the readers. I will remain eternally grateful.
Further thanks are due to the many contributors of data and figures for use in the book, including, again, Adrie Bos, Vasilis Pagonis, Nigel Poolton, and Sergey Sholom, plus Mark Akselrod, Ramona Gaza, Guerda Massilon, Kahli Remy, and Hannes Stadmann. I also thank my many collaborators throughout my career from whom I have learned so much and who have guided me on my own stumbling path through the topic. Thanks are also due to the editorial staff at Wiley for their professional guidance and assistance. Finally, I thank my many brilliant students who over the years have also taught me so much at the same time as I, hopefully, have taught them. Teaching is a two-way process, and I have loved every minute of it. I hope this book does them all justice.
Disclaimer
Reference to commercial products does not imply or represent endorsement of those products on the part of the author. It is noted that the author’s research has been funded at various points in his career by Landauer Inc. (USA) and Chiyoda Technol Corporation (Japan).
About the Companion Website
This book is accompanied by a companion website. www.wiley.com/go/mckeever/luminescence-measurements
This website includes: Exercises Figures Notes
Part I
Theory, Models, and Simulations
When … simulation and approximation yield similar results, the validity of the conclusions is strengthened.
– R. Chen and V. Pagonis 2014
1 Introduction
I consider then, that generally speaking, to render a reason of an effect or Phaenomenon, is to deduce it from something else in Nature more known than it self, and that consequently there may be divers kinds of Degrees of Explication of the same thing.
– R. Boyle 1669
1.1 How Did We Get Here?
Luminescence, the eerie glow of light emitted by many physical and biological substances, is familiar to us all. The bright speck of a firefly, the luminous glow from seawater in the evening, the glow of a watch dial in the dark – all are examples of luminescence phenomena that are familiar to most of us. Familiarity and understanding are not synonymous, however. Indeed, an understanding of the various luminescence phenomena has a very long genesis and over the centuries there have been several “divers kinds of Degrees of Explication”. Luminescence has had, and continues to have, practical uses in both every-day and in more esoteric applications. Computer screens, electronic indicators, lighting, lasers, and many, many other examples are indications that the field of luminescence is very broad and potentially very useful.
One such field of use is in the detection and measurement of radiation – a field generally known as “dosimetry,” or the act of measuring the dose of radiation absorbed by an object. The amount of radiation absorbed by an object and the subsequent amount of luminescence emitted from it is the basis of the use of luminescence in dosimetry. The connection between radiation and luminescence was made many years ago and, in fact, those of us active in the field of luminescence dosimetry can take pride in the fact that the study of luminescence can be traced to the beginning of the modern scientific method. Although it would be surprising if ancient Islamic or, perhaps, Chinese scholars had not already noted the phenomenon, in one of its many guises, it can nevertheless be argued that the first modern description of luminescence stems from the work of Robert Boyle in mid-seventeenth-century England, published in the Philosophical Transactions of the Royal Society. Boyle – considered to be the “father” of chemistry, as well as being a physicist, an inventor, a philosopher, and a theologian – gives an evocative description of (what we now term) luminescence emitted from a remarkable piece of diamond, loaned to him by a friend, John Clayton (Boyle 1664). The word “luminescence” was not used by Boyle who referred to it as the “glow” from the stone. In a later publication
A Course in Luminescence Measurements and Analyses for Radiation Dosimetry, First Edition. Stephen W.S. McKeever.
concerning luminescence from a liquid he uses the wonderfully suggestive term “self-shining” to describe the phenomenon (Boyle 1680).
Boyle’s 1664 account of luminescence from diamond is generally accepted as the first scientific description of the phenomenon of thermoluminescence (TL). Boyle described various ways of heating the diamond to induce from it the emission of light. It is not clear, however, how Boyle energized the diamond in the first place. We now know that the TL phenomenon requires that the material must first absorb energy from an external energy source. The energy thus stored is then released by the application of a second source of energy (heat). As the initial energy is released, some of it is emitted in the form of visible light (thermoluminescence). Without that first energy storage step, no TL can be induced. Boyle may or may not have known that the process he was observing was, in fact, a two-step procedure, but he was vague on how he energized the diamond in his possession; readers are left to speculate how this may have been achieved. Possibilities include natural radioactivity or light, but perhaps the most likely source was physical stimulation (rubbing, scratching, etc.) producing what we now call tribo-thermoluminescence (“tribo-” from the Greek “trībein,” meaning “to rub”). In any case, once heated to release the TL, the material would have to be energized again and energy stored a second time before the TL phenomenon could be seen again during heating.
We may never know in sufficient detail how Boyle treated his diamond to be able to answer this question with certainty – and perhaps we should be satisfied with leaving it as an intriguing mystery. For our purposes here, we can be satisfied that the phenomenon that we discuss in this book was first reported in such vivid and expressive terms as long ago as the mid-seventeenth century, and by such a luminary as Robert Boyle.
McKeever (1985) traces several pre-twentieth century published descriptions of luminescence stimulated by heating and indicates that the term “thermoluminescence” can probably be attributed to Eilhardt Wiedemann (Wiedemann 1889) in his work on the luminescence properties of a wide variety of materials. Following Wiedemann’s work, Wiedemann and Schmidt (1895) studied TL from an extensive series of materials following irradiation with electron beams, while Trowbridge and Burbank (1898), likewise, studied TL of fluorite following excitation by several different energy sources, including x-irradiation. These two early papers are examples where we can see the beginnings of the use of TL in radiation detection since, in each case, a source of radiation was used to provide the initial absorption of energy necessary for ultimate TL production. It is not surprising, therefore, to see the study of TL proceeding alongside the examination of radiation itself, with seminal works by Marie Curie and Ernest Rutherford, among others, including descriptions of thermoluminescence from minerals (Curie 1904; Rutherford 1913). Examinations of the color of the emitted light were also beginning around this time through studies of the spectra of the TL from various minerals (Morse 1905).
A point that should not go without mention is that Wiedemann (1889) and Wiedemann and Schmidt (1895) discussed the mechanism of luminescence in terms an “electric dissociation theory” wherein luminescence phenomena were explained on the basis of the separation and subsequent recombination of positive and negative charged species (specifically, positive and negative molecular ions). Others followed and adopted this initial and innovative suggestion to explain luminescence phenomena in a variety of materials (Nichols and Merritt 1912; Rutherford 1913). While the authors of the period attempted to apply this theory to all forms of luminescence, and while we now know that photoluminescence (i.e., fluorescence), for example, does not involve ionization and charge dissociation, the notion of charge dissociation and recombination nevertheless foreshadows our current understanding of the phenomena of TL, OSL, and phosphorescence. Bearing in mind that these early ideas initially suggested in the 1880s predate the birth of quantum mechanics, band theory, and the concepts of electron and hole generation, it is remarkable that the insight offered by these early pioneers aligns so
well with our current understanding of the latter phenomena, which is given in terms of the creation of negative electrons and positive holes, followed by their ultimate recombination.
As described in McKeever (1985), the use of TL in the study of radiation accelerated in the beginning decades of the twentieth century. A key area of research was to examine the relationship between the point defects within the materials studied (e.g. color centers) and their role in localizing (trapping) the electrons and holes ionized from their host atoms during the absorption of radiation. A feature of TL is that the luminescence at first increases and then decreases, forming a series of characteristic TL peaks as the temperature increases. It was realized that the cause of the TL peaks was the thermal release of trapped charge from lattice defects – with the larger the trapping energy, the higher the temperature of the TL peak. In 1930, in Vienna, Austria, Urbach discussed the connection between the energy needed to release the trapped charge and the TL peak position in a series of papers on luminescence from the alkali halides (Urbach 1930). However, it was not until the work of the group at the University of Birmingham in the United Kingdom that the relationship was quantified through the development of mathematical descriptions of the process (Randall and Wilkins 1945a, 1945b; Garlick and Gibson 1948).
Not long afterwards, Farrington Daniels and the research group at the University of Wisconsin, United States of America, discussed several applications in which TL could be a useful research tool. Among them was radiation dosimetry. Daniels and colleagues wrote: “Since in many crystals the intensity of thermoluminescence is nearly proportional to the amount of γ -radiation received, a considerable effort has been devoted to developing a practical means of measuring the exposure to gamma radiation.” (Daniels et al. 1953) – and so was born the field of thermoluminescence dosimetry. These authors specifically highlighted lithium fluoride as being the best crystal for this purpose and their work also initiated the parallel search for other TL dosimetry materials.
The growth of optically stimulated luminescence (OSL) as a method of radiation dosimetry had a similar genesis to that of TL and emerged as a potential dosimetry tool at about the same time. As described by Yukihara and McKeever (2011), the birth of OSL stems from the early work of the Becquerels, father and son, Edmond and Henri (E. Becquerel 1843; H. Becquerel 1883). These and similar studies through the late nineteenth and early twentieth centuries observed that phosphorescence could either be enhanced or quenched by the application of light to an irradiated material, the precise effect being dependent on the wavelength of the stimulating light. Observations of photoconductivity on some of these materials lead to the realization that free electrons were being produced during photostimulation and quenching of the phosphorescence (as discussed by Harvey 1957). Leverenz (1949) noted that when luminescence is enhanced by stimulating with an external light source, the eventual decay of the luminescence is unrelated to the characteristic fluorescence lifetime of the emitting species. As Leverenz (1949) states, for the luminescence to be produced, an “additional activation energy must be supplied to release the trapped electrons … This activation energy may be supplied by heat … or it may be supplied by additional photons.” When the energy is supplied by heat, TL results; when it is supplied by photons, OSL results.
It seems that the name, optically stimulated luminescence (OSL), appeared in the literature only in 1963 with the work of Fowler (Fowler 1963). Earlier names for the phenomenon included photophosphorescence, radiophotostimulation, photostimulation phosphorescence, co-stimulation phosphorescence, and photostimulated emission (see Yukihara and McKeever 2011). Even today, one often sees the phrase photostimulated luminescence (PSL) instead of OSL, the two names being synonymous, referring to the same phenomenon. For clarity, the more popular and most frequently used name of OSL will be used throughout this book.
As with TL, the connection between these optically stimulated effects and the initial absorption of energy from radiation was also established in the mid-twentieth century. The first