1996
DOI: 10.1006/spmi.1996.0079
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Interface roughness, polar optical phonons, and the valley current of a resonant tunneling diode

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Cited by 37 publications
(32 citation statements)
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“…Extrapolating the valley current to the limit of 0 K shows that 72 % of the valley current tends to be not thermally activated, but is most likely rather related to other elastic and inelastic electron scattering processes, such as interface roughness, alloy, and impurity scattering. [26][27][28] This result suggests that the thermally-activated tunnelling is not as significant in these InGaAs/AlAs/InP RTDs as previously thought. 29 It is important to note, however, that several material characteristics change with temperature, such as conduction band energy, accumulated stress, saturation velocity, and the incoherent scattering rate.…”
Section: Resultssupporting
confidence: 59%
“…Extrapolating the valley current to the limit of 0 K shows that 72 % of the valley current tends to be not thermally activated, but is most likely rather related to other elastic and inelastic electron scattering processes, such as interface roughness, alloy, and impurity scattering. [26][27][28] This result suggests that the thermally-activated tunnelling is not as significant in these InGaAs/AlAs/InP RTDs as previously thought. 29 It is important to note, however, that several material characteristics change with temperature, such as conduction band energy, accumulated stress, saturation velocity, and the incoherent scattering rate.…”
Section: Resultssupporting
confidence: 59%
“…One was the need to model extended devices through novel boundary conditions [55] which includes quantum charge selfconsistency and strong ineleastic scattering or quasi equilibrium in the contacts. The second key insight is that inelastic scattering from acoustic and polar optical phonons, alloy disorder, and interface roughness in the central device region can be modeled quantitatively in NEGF [56][57][58][59] and compare well to the valley currents in experimental data at low temperatures. At room temperature, however, a very different physics explains the typical high performance, high current density resonant tunneling diode valley current: It is thermionic emission through excited states.…”
Section: Physical Modelsmentioning
confidence: 73%
“…However, even at high temperatures, new islands nucleate on top of existing ones prior to full coalescence of the first layer. As a result, it is difficult to create an atomically-flat surface, which is desirable for making layered devices [42]. Time-varying process conditions may yield smoother interfaces than any constant input.…”
Section: Example: High-dimensional Kmc Simulationmentioning
confidence: 99%