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- W2007236872 abstract "A scaling argument for the conductance G of a disordered electronic system permits interpolation for the behavior of G between the localized and extended limits. For dimensionality d>2, there is a mobility edge at which the conductivity goes continuously to zero. At d=2, there is no true metallic conduction; the conductivity goes smoothly from logarithmic to exponential decrease with sample size L. A perturbation calculation confirms the ℓn L behavior for weak disorder. At finite temperature T and electric field E, effective length scales depending upon T and E are derived on the basis of relaxation and heating models for purposes of comparison with experiments on thin films. These show non-ohmic ℓn T and ℓn E contributions to the conductivity." @default.
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- W2007236872 modified "2023-10-16" @default.
- W2007236872 title "Scaling theory of localization and non-ohmic effects in two dimensions" @default.
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- W2007236872 doi "https://doi.org/10.1016/0022-3093(80)90566-9" @default.
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