1970
DOI: 10.1016/0022-3697(70)90001-6
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Monte Carlo determination of electron transport properties in gallium arsenide

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Cited by 845 publications
(159 citation statements)
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“…We ignored the impurity scattering in the quantum well, since the channel is not considerably doped. The scattering rates for 3D electrons are the same as those given by Fawcett et al 27 Velocity-field characteristics for Ga 0.51 In 0.49 P/ In x Ga 1Ϫx As/GaAs modulation doped heterostructures with different channel In mole fractions (x) are shown in Fig. 4.…”
Section: Effects Of Screening On Transport Propertiesmentioning
confidence: 94%
“…We ignored the impurity scattering in the quantum well, since the channel is not considerably doped. The scattering rates for 3D electrons are the same as those given by Fawcett et al 27 Velocity-field characteristics for Ga 0.51 In 0.49 P/ In x Ga 1Ϫx As/GaAs modulation doped heterostructures with different channel In mole fractions (x) are shown in Fig. 4.…”
Section: Effects Of Screening On Transport Propertiesmentioning
confidence: 94%
“…The procedure is similar to what is used for high-field transport Monte Carlo simulations in semiconductors. 4 In order to simulate an infinite, macroscopically homogeneous, system the cube is repeated periodically. The simulation is performed independently for all electrons and their displacement (xl, x2, xa) from the initial position os recorded at fixed time intervals At up to a total time T. From the simulation < xi > shows a linear dependence upon time, t, as predicted by the diffusion theory, and the diffusion constant along a direction xi is then obtained by means of the equation…”
Section: Transportmentioning
confidence: 99%
“…1). Of central importance is the fact that, were it not for the comparative inefficiency of the scattering mechanisms in the central valley in removing energy from the electrons present, the transferred electron effect would be nowhere near so obvious in GaAs as it is (Fawcett et al 1970). A second helpful property of GaAs is tnat crystals of the material can be grown semi-insulating (~10 8 Q cm), thereby making available to the device engineer a nominally nonconducting substrate upon which useful devices can be built from doped layers, grown either by epitaxy or by annealed ion implantation (Rees 1980).…”
Section: Introductionmentioning
confidence: 99%