Numéro |
J. Phys. I France
Volume 4, Numéro 10, October 1994
|
|
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Page(s) | 1373 - 1378 | |
DOI | https://doi.org/10.1051/jp1:1994193 |
J. Phys. I France 4 (1994) 1373-1378
Short Communication
Effect of coupling to the leads on the conductance fluctuations in one-dimensional disordered, mesoscopic systems
Asok K. Sen and S. GangopadhyayLow Temperature Physics Section, Saha Institute of Nuclear Physics, 1/AF, Bidhannagar, Calcutta 700 064, India
(Received 22 November 1993, revised 21 June 1994, accepted 28 July 1994)
Abstract
We study the electronic transport in a one-dimensional disordered chain with both
site-diagonal and off-diagonal (hopping) disorder, the latter being perfectly correlated to
the diagonal disorder at the nearest neighbor sites in a linear fashion. Since we allow the
hopping in the perfect leads to be different from the average hopping in the sample, the
average two-probe conductance (
< g >) and the conductivity (
) decay
non-monotonically with length. Because the peak regions of conductivity represent nearly
constant
s, these domains are quasi-Ohmic with their "effective" mean free
paths equal to the stationary values of
in these domains. Indeed, when
< g >
passes through these quasi-Ohmic regions, the standard deviation of
g latches on to almost
constant values of about
0.3e2/h, appropriate for 1D (as observed by us in a recent
paper). The evolution of the probability distribution
P(g) with length demonstrates that it
is unusually broad (nearly uniform) around the first quasi-diffusive regime and that for
larger lengths,
P(g) narrows down in general, but becomes non-monotonically broader
whenever
peaks up again, i.e., around the other (than the first) quasi-diffusive
regimes.
© Les Editions de Physique 1994