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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書目名稱Many-Body Theory of Solids影響因子(影響力)




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書目名稱Many-Body Theory of Solids網(wǎng)絡(luò)公開度學(xué)科排名




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Quantization of Waves (Second Quantization),ompton effect, photoelectric effect, infrared catastrophe, etc.), yet the wave nature of particles and the Schr?dinger 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