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Walter A. Harrison - Solid State Theory

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Walter A. Harrison Solid State Theory
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    Solid State Theory
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Solid State Theory: summary, description and annotation

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A well-written text . . . should find a wide readership, especially among graduate students. Dr. J. I. Pankove, RCA.
The field of solid state theory, including crystallography, semi-conductor physics, and various applications in chemistry and electrical engineering, is highly relevant to many areas of modern science and industry. Professor Harrisons well-known text offers an excellent one-year graduate course in this active and important area of research. While presenting a broad overview of the fundamental concepts and methods of solid state physics, including the basic quantum theory of solids, it surpasses more theoretical treatments in its practical coverage of physical applications. This feature makes the book especially useful to specialists in other fields who many encounter solid state problems in their own work. At least one year of quantum mechanics is required; however, the author introduces more advanced methods as needed.
Because virtually all of the properties of solids are determined by the valence electrons, the author devotes the first third of the book to electron states, including solid types and symmetry, band structure, electron dynamics, the self-consistent-field approximation, energy-band calculations, semi-conductor and semi-metal bands, impurity states, the electronic structure of liquids, and other topics. Dr. Harrison then turns to a more systematic treatment of the electronic properties of solids, focusing on thermodynamic properties, transport properties (including the Boltzmann equation), semi-conductor systems, screening, optical properties, the Landau theory of Fermi liquids, and amorphous semi-conductors.
In the final two chapters, Professor Harrison offers a cogent treatment of lattice vibrations and atomic properties and cooperative phenomena (magnetism and superconductivity). In addition to traditional background information, the book features penetrating discussions of such currently active problems as the Mott transition, the electronic structure of disordered systems, tunneling the Kondo effect, and fluctuation near critical points. In an important sense, the entire text constitutes a major vehicle for the clarification of quantum mechanics, resulting from, among other factors, a comparison of the semi-classical (Boltzmann equation) treatment of screening and the corresponding quantum (Liouville equation) treatment.

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Copyright 1979 by The Harrison Family Trust All rights reserved This Dover - photo 1
Copyright 1979 by The Harrison Family Trust All rights reserved This Dover - photo 2

Copyright 1979 by The Harrison Family Trust.

All rights reserved.

This Dover edition, first published in 1980, is an unabridged and corrected republication of the work originally published in 1970 by McGraw-Hill, Inc.

9780486152233

Library of Congress Catalog Card Number: 79-56032

Manufactured in the United States by Courier Corporation
63948709
www.doverpublications.com

TO LUCKY AND TO MY BOYS,
Rick, John, Will and Rob

PREFACE

This manuscript has been designed to serve as a text for a one-year graduate course in solid state theory. A year of quantum mechanics is prerequisite (more advanced methods are introduced as needed) but introductory solid state is not. Thus the course attempts to span the subject matter which in many universities is covered in an introductory solid state course and in a quantum theory of solids course. As an alternative to such a two-year program, Stanford offers this one general course and a number of shorter courses on specific topics in solid state.

In this one-year program I attempt to develop a sufficient familiarity with the concepts and methods of solid state physics that a reader will feel moderately at home in any solid state seminar or when reading any article in solid state physics. I attempt also to eliminate the threshold which may prevent a specialist in another field from attacking a solid state problem which arises in the context of his own work. Both these objectives, in my view, can be accomplished in a single year of study.

In this context there are very few topics in traditional or modern solid state physics which can be omitted altogether. Yet the subject is much too broad for any kind of complete coverage in a single course. An attempt to resolve this dilemma has been made by developing the fundamental ideas and approaches in many areas but this necessitates giving only a very small number of detailed applications. The first chapter develops the fundamentals of group and representation theory and gives only three illustrative applications (though use is made of group theory at many points later in the text). In discussing band structure only one prototype in each category is considered. The transport equation is derived, but is applied to only a few properties. Included, when possible, are discussions of currently active problems such as the Mott transition, the electronic structure of disordered systems, tunneling, the Kondo effect, and fluctuations near critical points. Which topics are most active vary from year to year and few remain of central interest indefinitely. Their inclusion, however, adds an air of relevance to the subject matter and brings the reader to the frontiers of knowledge in a number of areas.

Because virtually all of the properties of solids are determined by the valence electrons, I have focused on electron states in much of the first third of the text. This is predominantly a formulation of the approximate descriptions in different systems which allow a treatment of properties rather than a discussion of the energy bands themselves; the latter provide the basis for the treatment of very few properties. The remaining portion of the text is devoted to discussions of solids and liquids using these approximate descriptions. This organization of the material allows parallel treatments of each property for metals, semiconductors, and insulators, though in some cases it separates the discussion of related properties in one material. Throughout the text emphasis is placed on self-consistent-field methods for the treatment of interaction among electrons and pseudopotential methods for the treatment of the interaction among electrons and ions.

The timing of this course in the graduate curriculum and the breadth of its coverage can make it a vehicle for a major clarification of quantum mechanics for the student. Such clarification comes in the comparison of the semiclassical (Boltzmann equation) treatment of screening and the corresponding quantum (Liouville equation) treatment. It comes in understanding of the breakdown of the Franck-Condon principle and it comes with the understanding of off-diagonal long-range order in vibrating lattices and in superconductivity.

A course at this level also provides an opportunity to present two impressive phenomenologies, the Landau theory of Fermi liquids and the Ginsburg-Landau theory of superconductivity. Both of these are presented in the spirit in which they were generated rather than as consequences of microscopic theories. This form of presentation seemed much more in tune with an effort to enable students to generate good physics rather than to simply use the physics of others.

Throughout, an attempt is made to maintain a balance between the physics and the mathematics of our understanding of solids. Where the theory provides general methods for treating solids, the attempt has been to make the derivations careful and complete. Where the physical concepts are in my belief central, the tendency is only to outline the mathematical analysis. In some cases the details are shifted to the problems following each chapter; in some cases the reader may go to the more complete discussions referred to. Sufficient completeness in most arguments is presented, however, (frequently more complete than the original source) so that the references are more likely to provide additional applications than clarification of the methods.

In total, I view this as a text in physics rather than in mathematical methods. The emphasis is on current problems and modern concepts, but the traditional background which provides the foundation for modern theory is also included. My desire is to provide a framework that the reader can fill in with his subsequent reading and work, and upon which he can build understanding where it does not exist today.

Walter A. Harrison

Table of Contents

I
SOLID TYPES AND SYMMETRY
1. Crystal Structures

A familiar and useful classification of solids is by their electrical properties. We divide all materials into those which conduct and those which insulate. Metals are of course the classic conductors and ionic crystals are the classic insulators. Typically a metal will carry a large current when a voltage is applied across it. For a given voltage the current carried will decrease when the temperature is increased. An insulator, in contrast, will carry a negligible current for comparable voltages. Between these two extremes there are also semimetals and semiconductors. A semimetal, like a metal, will carry current and as in a metal that current will decrease as the temperature is increased. A semimetal is distinguished from a metal by the much smaller number of electronic carriers in a semimetal (smaller by a factor of perhaps 104). A semiconductor behaves as an insulator at low temperatures but will carry a current that increases as the temperature increases at fixed voltage.

We will see in detail how these differing electrical properties arise from the specific electronic structure. For the moment we may simply use the electrical properties as a criterion for distinguishing solids.

Each of these four solid types is characterized by a rather specific crystalline structure, or arrangement of constituent atoms. The exact details of the structure appear not to be the determining factor in the properties of solids, but it will be useful for our later considerations to discuss the typical structures and to consider those aspects of the properties which are determined by structure alone.

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