Abstract:We present a general formalism based on scattering theory to calculate quantum correlation functions involving several time-dependent current operators. A key ingredient is the causality of the scattering matrix, which allows one to deal with arbitrary correlation functions. The formalism proves useful, e.g., in view of recent developments in full counting statistics of charge transfer, where detecting schemes have been proposed for measurement of frequency dependent spectra of higher moments. Some of these sc… Show more
“…In [7] the discrepancy was claimed to be entirely due to the difference existing between unordered and T -ordered correlators [9,4]. Our explanation is different, as we spell out momentarily.…”
Section: Introductionmentioning
confidence: 64%
“…Second, we will present a model of energy independent scattering, where that difference matters. Though the model is implicit in previous works [2,5,7], its formalization allows to establish the equivalence between the in/out-and the T * -ordering of currents and hence between the two approaches mentioned at the beginning.…”
Section: Introductionmentioning
confidence: 99%
“…This remark being made, the scattering amplitude from |t 1 , α 1 to |t 2 , α 2 is denoted by S α 2 α 1 (t 2 − t 1 ). Equivalence between in/outand T -ordering has been shown [10,7] under the assumption that the scattering matrix satisfies S(t) = 0 , (t ≤ 0) .…”
Section: Introductionmentioning
confidence: 99%
“…An application of these findings is the clarification of a discrepancy between [8] and [7] concerning the third cumulant of charge transfer through a tunnel junction. In [7] the discrepancy was claimed to be entirely due to the difference existing between unordered and T -ordered correlators [9,4].…”
The basic quantum mechanical relation between fluctuations of transported charge and current correlators is discussed. It is found that, as a rule, the correlators are to be time-ordered in an unusual way. Instances where the difference with the conventional ordering matters are illustrated by means of a simple scattering model. We apply the results to resolve a discrepancy concerning the third cumulant of charge transport across a tunnel junction.
“…In [7] the discrepancy was claimed to be entirely due to the difference existing between unordered and T -ordered correlators [9,4]. Our explanation is different, as we spell out momentarily.…”
Section: Introductionmentioning
confidence: 64%
“…Second, we will present a model of energy independent scattering, where that difference matters. Though the model is implicit in previous works [2,5,7], its formalization allows to establish the equivalence between the in/out-and the T * -ordering of currents and hence between the two approaches mentioned at the beginning.…”
Section: Introductionmentioning
confidence: 99%
“…This remark being made, the scattering amplitude from |t 1 , α 1 to |t 2 , α 2 is denoted by S α 2 α 1 (t 2 − t 1 ). Equivalence between in/outand T -ordering has been shown [10,7] under the assumption that the scattering matrix satisfies S(t) = 0 , (t ≤ 0) .…”
Section: Introductionmentioning
confidence: 99%
“…An application of these findings is the clarification of a discrepancy between [8] and [7] concerning the third cumulant of charge transfer through a tunnel junction. In [7] the discrepancy was claimed to be entirely due to the difference existing between unordered and T -ordered correlators [9,4].…”
The basic quantum mechanical relation between fluctuations of transported charge and current correlators is discussed. It is found that, as a rule, the correlators are to be time-ordered in an unusual way. Instances where the difference with the conventional ordering matters are illustrated by means of a simple scattering model. We apply the results to resolve a discrepancy concerning the third cumulant of charge transport across a tunnel junction.
“…27 within the framework of scattering theory, 2 we can obtain an explicit expression of ⌳ ͑3͒ in terms of the transmission eigenvalues T n and of the voltage bias V across the junction. In particular, in the case of energy-independent scattering and in the limit of zero temperature of the noise source, we obtain…”
Under appropriate conditions, controllable two-level systems can be used to detect the third moment of current fluctuations. We derive a master equation for a quantum system coupled to a bath valid to the third order in the coupling between the system and the environment. In this approximation the reduced dynamics of the quantum system depends on the frequency-dependent third moment. Specializing to the case of a controllable two-level system ͑a qubit͒ and in the limit in which the splitting between the levels is much smaller than the characteristic frequency of the third moment, it is possible to show that the decay of the qubit has additional oscillations whose amplitude is directly proportional to the value of the third moment. We discuss an experimental setup where this effect can be seen.
International audienceThe impact of bound states in Landauer-Buttiker scattering approach tonon-equilibrium quantum transport is investigated. We show that the noise powerat frequency $\nu$ is sensitive to all bound states with energies $\omega_b$satisfying $|\omega_b| < \nu$. We derive the exact expression of the boundstate contribution and compare it to the one produced by the scattering statesalone. It turns out that the bound states lead to specific modifications ofboth space and frequency dependence of the total noise power. The theoreticaland experimental consequences of this result are discussed
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