Titlebook: Quantum Kinetic Theory and Applications; Electrons, Photons, Fedir T. Vasko,Oleg E. Raichev Book 2005 Springer-Verlag New York 2005 Boson.

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偽善

Interacting Phonon Systems,eracting phonon modes. Besides, the relaxation properties of the phonon system often control the energy and momentum transfer from non-equilibrium electrons to the lattice. Therefore, the kinetics of interacting phonons deserves a special consideration. Below we derive and analyze the kinetic equati

HEW

Effects of Electron-Electron Interaction, equation is derived here under the assumption of weak electron-electron interaction. One should take into account that there are important physical situations when this assumption is not valid, and the electron-electron interaction rebuilds the ground state of the electron system and changes the na

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Non-Equilibrium Electrons,purity system considered in Chapter 2. However, a consideration of electron scattering with emission or absorption of bosons leads to a more sophisticated collision integral, because the Pauli principle is essential for inelastic scattering. This kinetic equation is derived by analogy to the case of

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Non-Equilibrium Diagram Technique,ing, since both the reconstruction of energy spectrum and the distribution of quasiparticles have to be considered simultaneously. For these purposes, it is convenient to use the nonequilibrium diagram technique, which operates, apart from the retarded and advanced Green’s functions, with an additio

CLAMP

忘川河

Quantum Magnetotransport,the field and in the plane perpendicular to the field appears, and the kinetic coefficients are modified considerably if the cyclotron frequency exceeds the relaxation rate. Further qualitative modifications take place under the transition from the quasi-classical fields satisfying Eq. (9.35) to qua

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碎石頭

Multi-Channel Kinetics,t theory and can be described with the use of coupled kinetic equations for the distribution functions of these quasiparticles. There are, however, the cases when this approach is not valid, because the branches of energy spectrum are close to each other, and the consideration of non-diagonal (with