Physical review. B, Condensed matter · 1991 · 34 citations · 13 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsElectronic MaterialsMaterials PhysicsAlloysConductive MaterialsElectrical ConductivityElectrical Properties Of CeramicsMetalsPhase TransitionsElectrical Conductivity MeasurementsElectron-electron InteractionsInteraction EffectsMetal-insulator TransitionStrong Coupling EffectsTemperature Dependence Of ConductivityTemperature Dependence Of Electrical PropertiesTemperature-dependent Conductivity
We report the results of electrical conductivity [\ensuremath{\sigma}(T)] measurements in the temperature range 300>T>0.1 K on single crystals of tantalum-substituted sodium tungsten bronze (${\mathrm{Na}}_{\mathit{x}}$${\mathrm{Ta}}_{\mathit{y}}$${\mathrm{W}}_{1\mathrm{\ensuremath{-}}\mathit{y}}$${\mathrm{O}}_{3}$) with compositions near the metal-insulator transition (x-y\ensuremath{\approxeq}0.19). We find that over the entire temperature range investigated, strong interaction effects dominate the temperature dependences of \ensuremath{\sigma}(T). For samples that lie on the metallic side, the \ensuremath{\sigma}(T) values in the temperature range 4>T>0.3 K follow a power law in T with an exponent 1/3 and \ensuremath{\sigma}(T=0)\ensuremath{\approxeq}0.01${\mathrm{\ensuremath{\sigma}}}_{\mathrm{Mott}}$. This arises due to interaction effects in the critical regime, where the coherence length is very large due to the proximity to the metal-insulator transition. These samples below 0.3 K show signatures of a weak superconducting transition. The \ensuremath{\sigma}(T) of the insulating samples below 4 K either show correlated hopping behavior or follow a power law with \ensuremath{\sigma}(T=0)=0. At higher temperatures (T>10 K), the \ensuremath{\sigma}(T) of both types of samples show an almost linear dependence with T, which we suggest as arising from electron-phonon interactions.
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Patrick A. Lee, T. V. Ramakrishnan · Reviews of Modern Physics · 1985 · 6.1K citations
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