IEEE Transactions on Electron Devices · 1971 · 22 citations · 15 references
EngineeringElectrical EngineeringMicroelectronicsSemiconductor DevicesSemiconductor MaterialsCarrier TransportCharge Carrier TransportDevice ModelingDopingHigh-frequency Semiconductor DevicesSemiconductor PhysicsCarrier DynamicsCarrier GenerationCarrier InjectionCarrier Transport In SemiconductorsCarrier Transport MechanismsCarrier Transport ModelingEfficiencyTransit-time Devices
It is well known that GaAs bulk-effect devices generate RF power by velocity-modulating the charge carriers. We have found through a small-signal analysis and computer simulations that RF power could also be generated by density modulation of the carriers if the diode is subcritically doped ( <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">n_{0}L<5\times10^{11}</tex> cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-2</sup> ) and carrier injection at the cathode is limited to appropriate values. This second power-generating mechanism is transit-time dependent and is optimum when the transit angle is approximately 3π/2. Under optimum conditions, when the two power-generating mechanisms are combined, the device efficiency exceeds what is predicted by the static velocity-electric field characteristic. Computer results indicate that for sinusoidal operation a peak-to-valley current ratio of 3 to 1 is achievable for an intrinsic peak-to-valley velocity ratio of 2.5 to 1. Experimental and computed results agree qualitatively.
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Schottky Emission Through Thin Insulating Films
P. R. Emtage, W. Tantraporn · Physical Review Letters · 1962 · 241 citations
BULK GaAs NEGATIVE CONDUCTANCE AMPLIFIERS
Alan L. McWhorter, A.G. Foyt · Applied Physics Letters · 1966 · 64 citations