Quantum Statistical Theory of Superconductivity www.com SELECTED TOPICS IN SUPERCONDUCTIVITY Series Editor: Stuart Wolf Naval Research Laboratory Washington, D. CASE STUDIES IN SUPERCONDUCTING MAGNETS Design and Operational Issues Yukikazu Iwasa INTRODUCTION TO HIGH-TEMPERATURE SUPERCONDUCTIVITY Thomas P. Sheahen THE NEW SUPERCONDUCTORS Frank J. Owens and Charles P.
QUANTUM STATISTICAL THEORY OF SUPERCONDUCTIVITY Shigeji Fujita and Salvador Godoy STABILITY OF SUPERCONDUCTORS Lawrence Dresner A Continuation Order Plan is available for this series. A continuation order will bring delivery of each new volume immediately upon publication. Volumes are billed only upon actual shipment. For further information please contact the publisher.com Quantum Statistical Theory of Superconductivity Shigeji Fujita SUNY, Buffalo Buffalo, New York and Salvador Godoy Universidad Nacional Autonoma de México México, D., México Kluwer Academic Publishers NEW YORK, BOSTON , DORDRECHT, LONDON , MOSCOW www.com eBook ISBN 0-306- 47068-3 Print ISBN 0-306-45363-0 ©2002 Kluwer Academic Publishers New York, Boston, Dordrecht, London, Moscow All rights reserved No part of this eBook may be reproduced or transmitted in any form or by any means, electronic, mechanical, recording, or otherwise, without written consent from the Publisher Created in the United States of America Visit Kluwer Online at: http://www.com and Kluwer's eBookstore at: http://www.com Preface to the Series Since its discovery in 1911, superconductivity has been one of the most interesting topics in physics.
Superconductivity baffled some of the best minds of the 20th century and was finally understood in a microscopic way in 1957 with the landmark Nobel Prize-winning contribution from John Bardeen, Leon Cooper, and Robert Schrieffer. Since the early 1960s there have been many applications of superconductivity including large magnets for medical imaging and high-energy physics, radio-frequency cavities and components for a variety of applications, and quantum interference devices for sensitive magnetometers and digital circuits. These last devices are based on the Nobel Prize-winning (Brian) Josephson effect. In 1987, a dream of many scientists was realized with the discovery of superconducting compounds containing copper–oxygen layers that are superconducting above the boiling point of liquid nitrogen.
The revolutionary discovery of superconductivity in this class of compounds (the cuprates) won Georg Bednorz and Alex Mueller the Nobel Prize. This series on Selected Topics in Superconductivity will draw on the rich history of both the science and technology of this field. In the next few years we will try to chronicle the development of both the more traditional metallic superconductors as well as the scientific and technological emergence of the cuprate superconductors. The series will contain broad overviews of fundamental topics as well as some very highly focused treatises designed for a specialized audience.com This page intentionally left blank.com Preface Superconductivity is a striking physical phenomenon that has attracted the attention of physicists, chemists, engineers, and also the nontechnical public.
The theory of super- conductivity is considered difficult. Lectures on the subject are normally given at the end of Quantum Theory of Solids, a second-year graduate course. In 1957 Bardeen, Cooper, and Schrieffer (BCS) published an epoch-making mi- croscopic theory of superconductivity. Starting with a Hamiltonian containing electron and hole kinetic energies and a phonon-exchange-pairing interaction Hamiltonian, they demonstrated that (1) the ground-state energy of the BCS system is lower than that of the Bloch system without the interaction, (2) the unpaired electron (quasi-electron) has an energy gap ∆ 0 at 0 K, and (3) the critical temperature Tc can be related to ∆ 0 by 2 ∆ 0 = 3.53 k B Tc , and others.
A great number of theoretical and experimental investiga- tions followed, and results generally confirm and support the BCS theory. Yet a number of puzzling questions remained, including why a ring supercurrent does not decay by scattering due to impurities which must exist in any superconductor; why monovalent metals like sodium are not superconductors; and why compound superconductors, in- cluding intermetallic, organic, and high-T c superconductors exhibit magnetic behaviors different from those of elemental superconductors. Recently the present authors extended the BCS theory by incorporating band struc- tures of both electrons and phonons in a model Hamiltonian. By doing so we were able to answer the preceding questions and others.
We showed that under certain specific conditions, elemental metals at low temperatures allow formation of Cooper pairs by the phonon exchange attraction. These Cooper pairs, called the pairons, for short, move as free bosons with a linear energy–momentum relation. They neither overlap in space nor interact with each other. Systems of pairons undergo Bose–Einstein condensations in two and three dimensions.
The supercondensate in the ground state of the generalized BCS system is made up of large and equal numbers of ± pairons having charges ±2e, and it is electrically neutral. The ring supercurrent is generated by the ± pairons condensed at a single momentum q n = 2π n L – 1 , where L is the ring length and n an integer. The macroscopic supercurrent arises from the fact that ± pairons move with different speeds. Josephson effects are manifestations of the fact that pairons do not interact with each other and move like massless bosons just as photons do.
Thus there is a close analogy between a supercurrent and a laser. All superconductors, including high-T c cuprates, can be treated in a unified manner, based on the generalized BCS Hamiltonian.com viii PREFACE Because the supercondensate can be described in terms of independently moving pairons, all properties of a superconductor, including ground-state energy, critical tem- perature, quasi-particle energy spectra containing gaps, supercondensate density, specific heat, and supercurrent density can be computed without mathematical complexities. This simplicity is in great contrast to the far more complicated treatment required for the phase transition in a ferromagnet or for the familiar vapor–liquid transition. The authors believe that everything essential about superconductivity can be pre- sented to beginning second-year graduate students.
Some lecturers claim that much physics can be learned without mathematical formulas, that excessive use of formulas hinders learning and motivation and should therefore be avoided. Others argue that learning physics requires a great deal of thinking and patience, and if mathematical expressions can be of any help, they should be used with no apology. The average physics student can learn more in this way. After all, learning the mathematics needed for superconductor physics and following the calculational steps are easier than grasping basic physical concepts.
(The same cannot be said about learning the theory of phase transitions in ferromagnets.) The authors subscribe to the latter philosophy and prefer to develop theories from the ground up and to proceed step by step. This slower but more fundamental approach, which has been well-received in the classroom, is followed in the present text. Students are assumed to be familiar with basic differential, integral, and vector calculuses, and partial differentiation at the sophomore–junior level. Knowl- edge of mechanics, electromagnetism, quantum mechanics, and statistical physics at the junior–senior level are prerequisite.
A substantial part of the difficulty students face in learning the theory of supercon- ductivity lies in the fact that they need not only a good background in many branches of physics but must also be familiar with a number of advanced physical concepts such as bosons, fermions, Fermi surface, electrons and holes, phonons, Debye frequency, and density of states. To make all of the necessary concepts clear, we include five preparatory chapters in the present text. The first three chapters review the free-electron model of a metal, theory of lattice vibrations, and theory of the Bose–Einstein condensation. There follow two additional preparatory chapters on Bloch electrons and second quantization formalism.
Chapters 7–11 treat the microscopic theory of superconductivity. All basic thermodynamic properties of type I superconductors are described and discussed, and all important formulas are derived without omitting steps. The ground state is treated by closely following the original BCS theory. To treat quasi-particles including Bloch electrons, quasi-electrons, and pairons, we use Heisenberg’s equation-of-motion method, which reduces a quantum many-body problem to a one-body problem when the system- Hamiltonian is a sum of single-particle Hamiltonians.
No Green’s function techniques are used, which makes the text elementary and readable. Type II compounds and high-Tc superconductors are discussed in Chapters 12 and 13, respectively. A brief summary and overview are given in the first and last chapters. In a typical one-semester course for beginning second-year graduate students, the authors began with Chapter 1, omitted Chapters 2–4, then covered Chapters 5–11 in that order.
Material from Chapters 12 and 13 was used as needed to enhance the student’s interest. Chapters 2–4 were assigned as optional readings. The book is written in a self-contained manner so that nonphysics majors who want to learn the microscopic theory of superconductivity step by step in no particular hurry www.com PREFACE ix may find it useful as a self-study reference. Many fresh, and some provocative, views are presented.
Researchers in the field are also invited to examine the text. Problems at the end of a section are usually of a straightforward exercise type directly connected to the material presented in that section. By solving these problems, the reader should be able to grasp the meanings of newly introduced subjects more firmly. The authors thank the following individuals for valuable criticism, discussion, and readings: Professor M.
de Llano, North Dakota State University; Professor T. George, Washington State University; Professor A. Suzuki, Science University of Tokyo; Dr. Ko, Rancho Palos Verdes, California; Dr.
Watanabe, Hokkaido University, Sapporo. They also thank Sachiko, Amelia, Michio, Isao, Yoshiko, Eriko, George Redden, and Brent Miller for their encouragement and for reading the drafts. We thank Celia García and Benigna Cuevas for their typing and patience. We specially thank César Zepeda and Martin Alarcón for their invaluable help with computers, providing software, hardware, as well as advice.
One of the authors (S.) thanks many members of the Deparatmento de Física de la Facultad de Ciencias, Universidad Nacional Autónoma de México for their kind hospitality during the period when most of this book was written. Finally we gratefully acknowledge the financial support by CONACYT, México. Shigeji Fujita Salvador Godoy www.com This page intentionally left blank.com Contents Constants, Signs, and Symbols. Basic Experimental Facts.
Thermodynamics of a Superconductor. Development of a Microscopic Theory. Layout of the Present Book. Free-Electron Model for a Metal 2.
Conduction Electrons in a Metal; The Hamiltonian. Free Electrons; The Fermi Energy. Density of States. Heat Capacity of Degenerate Electrons 1; Qualitative Discussions.
Heat Capacity of Degenerate Electrons 2; Quantitative Calculations. Ohm’s Law, Electrical Conductivity, and Matthiessen’s Rule. Motion of a Charged Particle in Electromagnetic Fields. Lattice Vibrations: Phonons 3.
Lattice Vibrations; Einstein’s Theory of Heat Capacity. Oscillations of Particles on a String; Normal Modes. Transverse Oscillations of a Stretched String. Debye’s Theory of Heat Capacity.
Liquid Helium: Bose–Einstein Condensation 4. Free Bosons; Bose–Einstein Condensation. Bosons in Condensed Phase .com xii CONTENTS Chapter 5. Bloch Electrons; Band Structures 5.
The Bloch Theorem. The Kronig–Penney Model. Independent-Electron Approximation; Fermi Liquid Model. The Fermi Surface.
Electronic Heat Capacity; The Density of States. de-Haas–van-Alphen Oscillations; Onsager’s Formula. The Hall Effect; Electrons and Holes. Newtonian Equations of Motion for a Bloch Electron.
Bloch Electron Dynamics. Second Quantization; Equation-of-Motion Method 6. Creation and Annihilation Operators for Bosons. Physical Observables for a System of Bosons.
Creation and Annihilation Operators for Fermions. Second Quantization in the Momentum (Position) Space. Reduction to a One-Body Problem. One-Body Density Operator; Density Matrix.
Energy Eigenvalue Problem. Quantum Statistical Derivation of the Fermi Liquid Model. Interparticle Interaction; Perturbation Methods 7. Electron–Ion Interaction; The Debye Screening.
Electron–Electron Interaction. More about the Heat Capacity; Lattice Dynamics. Electron–Phonon Interaction; The Fröhlich Hamiltonian. Perturbation Theory 1; The Dirac Picture.
Scattering Problem; Fermi’s Golden Rule. Perturbation Theory 2; Second Intermediate Picture. Electron–Impurity System; The Boltzmann Equation. Derivation of the Boltzmann Equation.
Phonon-Exchange Attraction. The Generalized BCS Hamiltonian. The Cooper Problem 1; Ground Cooper Pairs .