1985
DOI: 10.1103/physrevb.32.1955
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Metal-insulator transition in the compensated sodium bronze,NaxTay

Abstract: We have measured the dc electrical conductivity o of cubic Na"Ta"WI~03 from 1.6 to 295 K for various values of x and y. A sample with x -y=0. 18 appears to fall directly at the metal-insulator transition and shows an unusual temperature dependence, g(T)~T, -from 1.6 K to room temperature. A model for o. (T) based on the scaling theory of localization, when used to interpret the data on this and other samples, gives a conductivity exponent v of 1.0. This model assumes that o. (T) is controlled by a thermal smea… Show more

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Cited by 40 publications
(27 citation statements)
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“…9͒ show a transport behavior characteristic for systems near the metalinsulator transition, where the resistivity is inversely proportional with temperature. Dubson and Holcomb 21 derived the temperature dependence of the conductivity near the MIT point from the energy dependence of the zero-temperature conductivity properties around the Fermi level. When applied to hole transport, this temperature dependence is given by…”
Section: B High-temperature Behavior: T>t Cmentioning
confidence: 99%
“…9͒ show a transport behavior characteristic for systems near the metalinsulator transition, where the resistivity is inversely proportional with temperature. Dubson and Holcomb 21 derived the temperature dependence of the conductivity near the MIT point from the energy dependence of the zero-temperature conductivity properties around the Fermi level. When applied to hole transport, this temperature dependence is given by…”
Section: B High-temperature Behavior: T>t Cmentioning
confidence: 99%
“…Equation (37) predicts that resistivity due to spin disorder scattering is independent of temperature in the paramagnetic region, where hSi ¼ 0, if B ¼ 0. Then the experimentally observed increase in resistivity with decreasing temperature was explained by using a result derived by Dubson and Holcomb [27] for the T dependence of the resistivity near the metal insulator transition,…”
Section: Transport Propertiesmentioning
confidence: 99%
“…But the material remains insulating until x -y exceeds about 0.2 (Dubson and Holcomb 1985). Photoemission experiments confirm the localized nature of the states at small x -y and suggest that the disorder responsible for the localization is due to the Na, not to the random distribution of Wand Ta (Hollinger et al 1985).…”
Section: Localization By Disordermentioning
confidence: 56%