Distribution of conductance and its universal fluctuations in 1-D disordered, mesoscopic systems
Résumé
The evolution with length of the probability distribution for the two-probe conductance (g2) of a disordered one-dimensional system is obtained numerically. It evolves from a strongly peaked distribution close to g2=1 in the small length limit towards another strongly peaked distribution near g2=0 in the large length limit. In the middle it goes through a quasi-diffusive regime where the distribution is nearly uniform. This is consistent with a universal conductance fluctuation of magnitude $\cong$0.3 e2/h (as observed in a recent paper) occurs in such a domain.
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Origine : Accord explicite pour ce dépôt