New method for solving Boltzmann's equation for electrons in metals
New method for solving Boltzmann's equation for electrons in metals
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DOI:
10.1103/physrevb.17.3725
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发表时间:
1978-05
影响因子:
3.7
通讯作者:
P. B. Allen
中科院分区:
文献类型:
--
作者:
P. B. Allen
A new set of basis functions is introduced, consisting of products of Fermi-surface harmonics F J (k) and polynomials σ n (ε) in the energy (ε− μ) k B T. The former are orthonormal on the Fermi surface, and the latter are orthonormal with weight function−∂ f∂ ε. In terms of this set the exact semiclassical Boltzmann equation takes a particularly simple form, giving a matrix equation which can probably be truncated at low order to high accuracy. The connection with variational methods is simple. Truncating at a 1× 1 matrix gives the usual variational solution where φ k is assumed proportional to ν kx for electrical conductivity and (ε− μ) ν kx for thermal conductivity. Explicit equations are given for the matrix elements Q J n, J′ n′ of the scattering operator for the case of phonon scattering, and a perturbation formula for ρ is given which is accurate for weak anisotropy. The matrix elements are simple integrals over spectral functions α 2 (±, J, J′) F (Ω) which generalize the electron-phonon spectral function α 2 F (Ω) used in superconductivity theory. Analogies are described between Boltzmann theory and Eliashberg theory for T c of superconductors. The intimate relations between high-temperature resistance and the s-or p-wave transition temperature are made explicit.