Abstract:We address frequency-dependent quantum transport through mesoscopic conductors in the semiclassical limit. By generalizing the trajectory-based semiclassical theory of dc quantum transport to the ac case, we derive the average screened conductance as well as ac weak-localization corrections for chaotic conductors. Thereby we confirm respective random matrix results and generalize them by accounting for Ehrenfest time effects. We consider the case of a cavity connected through many leads to a macroscopic circui… Show more
“…The charge relaxation resistance has also been investigated for small metallic islands where the tunnel junction to the reservoir is described by a large number of weakly transmitting channels [53,54]. In this regime, a mapping to the problem of a single particle on a ring subject to dissipation has been exploited [55] to demonstrate a new fixed point at large transparency associated to the quantized resistance R q = h/e 2 .…”
We formulate a general approach for studying the low frequency response of an interacting quantum dot connected to leads in the presence of oscillating gate voltages. The energy dissipated is characterized by the charge relaxation resistance which, under the loose assumption of Fermi liquid behaviour at low energy, is shown to depend only on static charge susceptibilities. The predictions of the scattering theory are recovered in the non-interacting limit while the effect of interactions is simply to replace densities of states by charge susceptibilities in formulas. In order to substantiate the Fermi liquid picture in the case of a quantum RC geometry, we apply a renormalization-group analysis and derive the low energy Hamiltonian for two specific models: the Anderson and the Coulomb blockade models. The Anderson model is shown, using a field theoretical approach based on Barnes slave-bosons, to map onto the Kondo model. We recover the well-known expression of the Kondo temperature for the asymmetric Anderson model and compute the charge susceptibility. The Barnes slave-bosons are extended to the Coulomb blockade model where the renormalization-group analysis can be carried out perturbatively up to zero energy. All calculations agree with the Fermi liquid nature of the low energy fixed point and satisfy the Friedel sum rule.
“…The charge relaxation resistance has also been investigated for small metallic islands where the tunnel junction to the reservoir is described by a large number of weakly transmitting channels [53,54]. In this regime, a mapping to the problem of a single particle on a ring subject to dissipation has been exploited [55] to demonstrate a new fixed point at large transparency associated to the quantized resistance R q = h/e 2 .…”
We formulate a general approach for studying the low frequency response of an interacting quantum dot connected to leads in the presence of oscillating gate voltages. The energy dissipated is characterized by the charge relaxation resistance which, under the loose assumption of Fermi liquid behaviour at low energy, is shown to depend only on static charge susceptibilities. The predictions of the scattering theory are recovered in the non-interacting limit while the effect of interactions is simply to replace densities of states by charge susceptibilities in formulas. In order to substantiate the Fermi liquid picture in the case of a quantum RC geometry, we apply a renormalization-group analysis and derive the low energy Hamiltonian for two specific models: the Anderson and the Coulomb blockade models. The Anderson model is shown, using a field theoretical approach based on Barnes slave-bosons, to map onto the Kondo model. We recover the well-known expression of the Kondo temperature for the asymmetric Anderson model and compute the charge susceptibility. The Barnes slave-bosons are extended to the Coulomb blockade model where the renormalization-group analysis can be carried out perturbatively up to zero energy. All calculations agree with the Fermi liquid nature of the low energy fixed point and satisfy the Friedel sum rule.
“…Governing the crossover is the Ehrenfest time, which, when it is small compared to the average time spent inside the cavity, separates the two cases as in Definition 1. For larger Ehrenfest time, when RMT stops being applicable, the semiclassical treatment correspondingly becomes notably more complicated [18,19,30,56,57,68,69,72,73]. However, a particular way of partitioning the diagrams provided enough of a simplification that the contribution of all the leading order diagrams could be obtained [70].…”
Articles you may be interested inCombinatorial theory of the semiclassical evaluation of transport moments. I. Equivalence with the random matrix approach J. Math. Phys. 54, 112103 (2013) Electronic transport through chaotic quantum dots exhibits universal behaviour which can be understood through the semiclassical approximation. Within the approximation, calculation of transport moments reduces to codifying classical correlations between scattering trajectories. These can be represented as ribbon graphs and we develop an algorithmic combinatorial method to generate all such graphs with a given genus. This provides an expansion of the linear transport moments for systems both with and without time reversal symmetry. The computational implementation is then able to progress several orders further than previous semiclassical formulae as well as those derived from an asymptotic expansion of random matrix results. The patterns observed also suggest a general form for the higher orders. C 2013 AIP Publishing LLC.[http://dx
“…Equation (43) can be generalized to ac transport considered in Ref. 29 by including in the latter equation the -dependent factors given in (5) and (6). The result in (43) again splits into two parts, with the first involving the semiclassical moments M(n) calculated in Ref.…”
Section: A Moments Of Transmissionmentioning
confidence: 99%
“…This equation incorporates both (27) and (29). If we introduce the notation M[i,j ] ≡ max{t enc,i ,t enc,j }, we can then define the times t i = t i − M[kī,k i+1 ] as before (28).…”
Transport properties of open chaotic ballistic systems and their statistics can be expressed in terms of the scattering matrix connecting incoming and outgoing wave functions. Here we calculate the dependence of correlation functions of arbitrarily many pairs of scattering matrices at different energies on the Ehrenfest time using trajectory-based semiclassical methods. This enables us to verify the prediction from effective randommatrix theory that one part of the correlation function obtains an exponential damping depending on the Ehrenfest time, while also allowing us to obtain the additional contribution that arises from bands of always correlated trajectories. The resulting Ehrenfest-time dependence, responsible, e.g., for secondary gaps in the density of states of Andreev billiards, can also be seen to have strong effects on other transport quantities, such as the distribution of delay times.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.