2003
DOI: 10.1063/1.1568529
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Lateral current density fronts in asymmetric double-barrier resonant-tunneling structures

Abstract: We present a theoretical analysis and numerical simulations of lateral current density fronts in bistable resonant-tunneling diodes with Z-shaped current-voltage characteristics. The bistability is due to the charge accumulation in the quantum well of the double-barrier structure. We focus on asymmetric structures in the regime of sequential incoherent tunneling and study the dependence of the bistability range, the front velocity and the front width on the structure parameters. We propose a sectional design o… Show more

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Cited by 11 publications
(3 citation statements)
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References 22 publications
(43 reference statements)
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“…7 Specific functional forms f (a, u), j(a, u), and D a (a) have been derived for various semiconductors and semiconductor structures. 2,7,8,9,10,17,18,20,34,41,42 The physical meaning of a depends on the particular type of bistable structure: a corresponds to the bias of the emitter p -n junction for avalanche transistors, 18 thyristors 20 and thyristorlike structures, 21 interface charge for heterostructure hot electron diode, 34 electron charge stored in the quantum well for bistable double barrier resonant tunneling diode, 41,42 etc.…”
Section: Model Of a Bistable Semiconductor Systemmentioning
confidence: 99%
“…7 Specific functional forms f (a, u), j(a, u), and D a (a) have been derived for various semiconductors and semiconductor structures. 2,7,8,9,10,17,18,20,34,41,42 The physical meaning of a depends on the particular type of bistable structure: a corresponds to the bias of the emitter p -n junction for avalanche transistors, 18 thyristors 20 and thyristorlike structures, 21 interface charge for heterostructure hot electron diode, 34 electron charge stored in the quantum well for bistable double barrier resonant tunneling diode, 41,42 etc.…”
Section: Model Of a Bistable Semiconductor Systemmentioning
confidence: 99%
“…For samples with a large diameter, they predicted α = 1, while for samples with a small diameter they find α = 3/2. In related work on semiconductor systems, Schöll and co-workers introduced reaction-diffusion models for the lateral dynamics of the front that separates the high and low current density states for double barrier resonant tunneling structures [30] and superlattices [31].…”
Section: Introductionmentioning
confidence: 99%
“…In fact, we will show that the electronic transport in superlattices, which leads to current branches, can be approximated by an equivalent circuit consisting of tunnel diodes connected in series. Tunnel diodes are nonlinear circuit elements, with similar N -shaped currentvoltage characteristics as superlattices and double barrier resonant tunneling diodes (DBRT ) [17,18,3,19,20,21,22], which can also show a regime, where the current I decreases with increasing voltage V . This is depicted in Fig.…”
Section: Introductionmentioning
confidence: 99%