2006
DOI: 10.1007/s10825-006-7917-3
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From wave-functions to current-voltage characteristics: overview of a Coulomb blockade device simulator using fundamental physical parameters

Abstract: The purpose of this article is to present an accurate way, based on a physical description, to simulate

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Cited by 19 publications
(21 citation statements)
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References 17 publications
(17 reference statements)
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“…The method used in the code SENS to simulate QD-based single-electron devices has been described elsewhere for single- [27,28] and double-dot [29] DTJs or SETs [30]. Here, we just summarize briefly the main stages of the calculation.…”
Section: Modelmentioning
confidence: 99%
See 3 more Smart Citations
“…The method used in the code SENS to simulate QD-based single-electron devices has been described elsewhere for single- [27,28] and double-dot [29] DTJs or SETs [30]. Here, we just summarize briefly the main stages of the calculation.…”
Section: Modelmentioning
confidence: 99%
“…where S barr is a surface inside the tunnel barrier which separates arbitrarily the dot and the electrode domains [28], ψ d and ψ L are the wave functions in the QD and the lead, respectively, and m barr is the electron effective mass in the barrier. The wave function ψ L is deduced from an analytical expression derived within the WKB approximation, which has been proven correct in the simple case of a triangular barrier [28].…”
Section: Modelmentioning
confidence: 99%
See 2 more Smart Citations
“…To obtain accurate simulation results for these devices, the knowledge of transport mechanisms in a basic system composed of one quantum dot (here a silicon nanocrystal), embedded in an insulator (here silicon oxide) and connected to two metallic electrodes through tunnel barriers, is required. Whatever the level of accuracy of the physical description considered, the simulation of this type of device is usually based on the hypothesis that the tunnelling process is purely sequential [3]. In other words, it is assumed that the tunnel transfer of one electron through the oxide barriers is slow enough for the electron phase coherence to be systematically broken by inelastic scattering in the dot (e.g.…”
Section: Introductionmentioning
confidence: 99%