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Titlebook: Many-Body Theory of Solids; An Introduction John C. Inkson Book 1984 Plenum Press, New York 1984 electron.field theory.fields.many-body the

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书目名称Many-Body Theory of Solids
副标题An Introduction
编辑John C. Inkson
视频video
图书封面Titlebook: Many-Body Theory of Solids; An Introduction John C. Inkson Book 1984 Plenum Press, New York 1984 electron.field theory.fields.many-body the
描述here exists a gap in the present literature on quantum mechanics T and its application to solids. It has been difficult to find an intro­ ductory textbook which could take a student from the elementary quan­ tum mechanical ideas of the single-particle Schrodinger equations, through the formalism and new physical concepts of many-body theory, to the level where the student would be equipped to read the scientific literature and specialized books on specific topics. The present book, which I believe fills this gap, grew out of two courses which I have given for a number of years at the University of Cambridge: "Advanced Quan­ tum Mechanics," covering the quantization of fields, representations, and creation and annihilation operators, and "Many Body Theory," on the application of quantum field theory to solids. The first course is a final-year undergraduate physics course while the second is a joint first­ and fourth-year undergraduate math­ year postgraduate physics course ematics course. In an American context this would closely correspond to a graduate course at the masters level. In writing this book I have tried to stress the physical aspects of the mathematics preferring where
出版日期Book 1984
关键词electron; field theory; fields; many-body theory; mathematics; mechanics; physical concepts; physics; quanti
版次1
doihttps://doi.org/10.1007/978-1-4757-0226-2
isbn_softcover978-1-4757-0228-6
isbn_ebook978-1-4757-0226-2
copyrightPlenum Press, New York 1984
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Quantization of Waves (Second Quantization),ompton effect, photoelectric effect, infrared catastrophe, etc.), yet the wave nature of particles and the Schrödinger equation dominates most considerations from then on. In this chapter we will look at the particle nature of waves and begin the development of a unified approach to fields and parti
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Interacting Systems and Quasiparticles,move throughout the whole crystal. In quantum terms we would like to replace this, as far as possible, by a set of single-particle states (in the sense of the Hartree or Hartree-Fock approximation), so that we could calculate the various properties of the solid. The true eigenstates of the system ar
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The Normal System, we will consider the interacting electron gas in a solid. What we are interested in is to what extent the first-order terms in the various functions (polarization, self-energy, Green’s function) describe the properties of a real solid. To some extent we already know from the success of single-parti
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,Thermal Effects on the Green’s Function,tween the existence of inexact states in interacting quantum mechanics and the equipartition theorem in statistical mechanics. In fact, quantum statistical mechanics is based upon the same framework as classical statistical mechanics. For this reason we will not try to develop a detailed theory here
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Special Methods,ality, however, it is not always the most suitable method for any particular problem. The iteration series must be developed in many different directions in order to include the correct physical properties, and it is not always obvious which direction (or, alternatively, which subset of diagrams) wi
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