Metal-Insulator Transition in Quench-Condensed<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Al</mml:mi></mml:mrow><mml:mrow><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Ge</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>−</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>: "Scaling" and Tunneling Experiments
J. LesueurLaboratoire de Physique des Solides, Université de Paris Sud, Centre d'Orsay, 91405 Orsay, FranceL. DumoulinLaboratoire de Physique des Solides, Université de Paris Sud, Centre d'Orsay, 91405 Orsay, FranceP. NédellecUniversité Paris Cité
1985lv
ABI
Abstract
We report on the metal-insulator transition of quench-condensed ${\mathrm{Al}}_{x}{\mathrm{Ge}}_{1\ensuremath{-}x}$. The transition is obtained either by variation of $x$ or by low-temperature annealing (amorphous-relaxation-like process). This last approach gives a straightforward illustration of the scaling theory of localization and information about the critical behavior. Tunneling measurements of the correlation gap $\ensuremath{\Delta}$ allow a comparison with other materials and show strong electron interactions in this highly disordered system.
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