1999
DOI: 10.1103/physrevb.59.10748
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Quantum open-systems approach to current noise in resonant tunneling junctions

Abstract: A quantum Markovian master equation is derived to describe the current noise in resonant tunneling devices. This equation includes both incoherent and coherent quantum tunneling processes. We show how to obtain the population master equation by adiabatic elimination of quantum coherences in the presence of elastic scattering. We calculate the noise spectrum for a double well device and predict subshot noise statistics for strong tunneling between the wells. The method is an alternative to Green's function meth… Show more

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Cited by 63 publications
(36 citation statements)
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“…The details of how the quantum stochastic processes in the readout dot determine the average current though the readout dot are given in Ref. 12. The link with the stochastic formalism of Sec.…”
Section: Average Steady-state Propertiesmentioning
confidence: 99%
“…The details of how the quantum stochastic processes in the readout dot determine the average current though the readout dot are given in Ref. 12. The link with the stochastic formalism of Sec.…”
Section: Average Steady-state Propertiesmentioning
confidence: 99%
“…The second part represents the coupling to the leads, which can be derived fromĤ lead−dot using either Greens functions 9,22 or second order perturbation theory on the density operator 25 ,…”
Section: Modelmentioning
confidence: 99%
“…Our approach is based on a master equation for the transport through the dots combined with the quantum regression theorem 23 to calculate the shot noise in the manner originally developed in Refs. 24,25 .…”
mentioning
confidence: 99%
“…9 Given the barrier thickness of our samples, it is appropriate to see the tunneling process as sequential, a regime in which quantum and semi-classical models give the same answer. 10 The results of our calculations are summarized in Fig.4, where in a simulated three-dimensional plot we represent the Fano factor as a function of the ratios T 2 /T 1 and T 3 /T 1 (T i is the transmission probability through the i-th barrier, considered individually). If the tunneling probability through the emitter and collector barriers is the same, that is, T 3 = T 1 , and the central barrier is not thicker than either of the two end barriers (T 2 ≥ T 1 ) then, according to Fig.4, the minimum Fano factor should range between 0.41 (when T 2 =T 1 ) and 0.5 (when T 2 ≫ T 1 , that is, in the DBRT limit).…”
mentioning
confidence: 99%
“…10,11,12 A Triple Barrier Resonant Tunneling Diode (TBRTD) is in principle more suitable than a DBRTD to study the effect of coherence on noise since in the TBRTD the coupling between its two wells can be varied by adjusting the thickness of the middle barrier, while maintaining the low current necessary for noise measurements with thick end barriers.…”
mentioning
confidence: 99%