1996
DOI: 10.1103/physrevb.54.14423
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Divergence of classical trajectories and weak localization

Abstract: We study the weak localization correction (WLC) to transport coefficients of a system of electrons in a static long-range potential (e.g. an antidot array or ballistic cavity). We found that the weak localization correction to the current response is delayed by the large time tE = λ −1 | lnh|, where λ is the Lyapunov exponent. In the semiclassical regime tE is much larger than the transport lifetime. Thus, the fundamental characteristic of the classical chaotic motion, Lyapunov exponent, may be found by measur… Show more

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Cited by 214 publications
(436 citation statements)
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“…In contrast to the non-interacting problem, the currents to the left and right are now completely correlated. Equations (137) and (138) can be used to eliminate the voltage fluctuations. The result is conveniently expressed in the frequency representation,…”
Section: Noise Of a Capacitormentioning
confidence: 99%
See 1 more Smart Citation
“…In contrast to the non-interacting problem, the currents to the left and right are now completely correlated. Equations (137) and (138) can be used to eliminate the voltage fluctuations. The result is conveniently expressed in the frequency representation,…”
Section: Noise Of a Capacitormentioning
confidence: 99%
“…These developments are described in Section VI. 34 Exceptions are frequency dependent weak localization corrections [137] which depend in addition to the RC-time also on the dwell time [138], and perfect ballistic wires which have a charge neutral mode determined by the transit time as the lowest collective mode [139].…”
Section: Scattering Theory Of Frequencymentioning
confidence: 99%
“…. imp ) of a product of a retarded and advanced Green's functions, Following the standard route of the quasiclassical formalism 35,36,37 , we perform the Wigner transformation, 6) where R 1 = (r 4 + r 1 )/2, R 2 = (r 2 + r 3 )/2, r = r 4 − r 1 , and r ′ = r 2 − r 3 . Note that the factors depending on the vector potential make the ballistic diffuson (2.6) gaugeinvariant.…”
Section: General Formalism a Smooth Disordermentioning
confidence: 99%
“…This counter-intuitive feature, usually referred to as dynamical localization [7], was fully understood [8] after mapping the kicked rotor problem onto a short range one-dimensional disordered system where localization is well established. Deviations from the BGS conjecture are also expected [9] for eigenvalue separations δE ∼ /t E due to weak localization effects. The typical scale t E = λ −1 | log | is the Ehrenfest time with λ the classical Lyapunov exponent.…”
Section: Introductionmentioning
confidence: 84%