Pa. Mello et Hu. Baranger, Interference phenomena in electronic transport through chaotic cavities: an information-theoretic approach, WAVE RAND M, 9(2), 1999, pp. 105-146
We develop a statistical theory describing quantum-mechanical scattering of
a particle by a cavity when the geometry is such that the classical dynami
cs is chaotic. This picture is relevant to a variety of physical systems, r
anging from atomic nuclei to mesoscopic systems and microwave cavities; the
main application here is to electronic transport through ballistic microst
ructures. The theory describes the regime in which there are two distinct t
imescales, associated with a prompt and an equilibrated response, and is ca
st in terms of the matrix of scattering amplitudes S. The prompt response i
s related to the energy average of S which, through the notion of ergodicit
y, is expressed as the average over an ensemble of similar systems. We use
an information-theoretic approach: the ensemble of S matrices is determined
by (1) general physical features, such as symmetry, causality, and ergodic
ity, (2) the specific energy average of S, and (3) the notion of minimum in
formation in the ensemble. This ensemble, known as Poisson's kernel, is mea
nt to describe those situations in which any other information is irrelevan
t. Thus, one constructs the one-energy statistical distribution of S using
only information expressible in terms of S itself, without ever invoking th
e underlying Hamiltonian. This formulation has a remarkable predictive powe
r: from the distribution of S we derive properties of the quantum conductan
ce of cavities, including its average, its fluctuations, and its full distr
ibution in certain cases, both in the absence and in the presence of prompt
response. We obtain good agreement with the results of the numerical solut
ion of the Schrodinger equation for cavities in which the assumptions of th
e theory hold, namely, cavities in which either prompt response is absent o
r there are two widely separated timescales. Good agreement with experiment
al data is obtained once temperature-smearing and dephasing effects are tak
en into account.