Diffusion on the Fermi-Surface and the Conductivity of Metals
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概要
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The transport phenomena in metals, such as the electrical and the thermal conductivity, are treated as a kind of the diffusion of electrons on the Fermi-surface. Grüneisen's well-known formula is gained for the electrical conductivity $\sigma$, and as for the thermal conductivity $\kappa$ the expression $\kappa{=}\sigma T\frac{\pi^{2}}{3}\left(\frac{k}{e}\right)^{2}\bigg/\left\{1+\left(\frac{\theta}{T}\right)^{2}\left(\frac{K}{q_{0}}\right)^{2}\int_{0}^{\theta/T}\frac{x^{3}dx}{\mathrm{e}^{x}-\mathrm{e}^{-x}}\bigg/\int_{0}^{\theta/T}\frac{x^{5}dx}{(\mathrm{e}^{x}-1)(1-\mathrm{e}^{-x})}\right\}$ is obtained. In this equation $\theta$ denotes the Debye temperature, $K$ and $q_{0}$ are the maximum wave numbers of electrons and phonons respectively.
- INSTITUTE OF PURE AND APPLIED PHYSICSの論文
- 1953-05-25
著者
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TODA Morikazu
Institute of Physics, Tokyo University of Education
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Toda Morikazu
Instittes Of Physics Tokyo Bunrika University And Tokyo University
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- Diffusion on the Fermi-Surface and the Conductivity of Metals