ISSN:
1573-7357
Source:
Springer Online Journal Archives 1860-2000
Topics:
Physics
Notes:
Abstract Contrary to previous statements in the literature, large deviations from Matthiessen's rule in fine wiresare to be expected on the basis of a straight-forward solution of the ordinary transport equation, assuming the relaxation-time approximation and imposing the idealized condition of “diffuse” scattering of electrons at the boundaries. Using Chambers' path-integral method to evaluate the current density in a wire of arbitrary cross-sectional shape, the effects of boundary scattering on the resistivity in the regimed ≲0.1λ have been calculated for two model Fermi surface geometries. For the temperature-dependent part of the resistivity, Δρ d (T)≡ρ d (T)−ρ d (0), two distinct types of behavior are found in the alternative cases: (1) for a spherical Fermi surface, Δρ d(T) increases logarithmically with ρ d(0); (2) for a cylindrical Fermi surface, Δρ d (T) increases essentially linearly with ρ d (0). [In each case the qualitative dependence of ρ d(0) on λ/d is, for practical purposes, “linear.” However, the correct value of the product ρ∞λ in the cylindrical case is not simply given in the ordinary way by the slope of an empirical plot of ρ d (0) vs.d −1.] A comparison of theoretical results for the two simple models with the published data for indium and gallium shows that the actual temperature-dependent size effects are consistent, both qualitatively and, by a rough estimation, quantitatively, with the expected behavior.
Type of Medium:
Electronic Resource
URL:
http://dx.doi.org/10.1007/BF00660066
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