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In this paper, an investigation of the static/dynamic performance of dual-emitter phototransistors (DEPTs) as an electrooptical switch was made. In the static case, the measured optical gains (the collector photocurrents) of DEPTs operated at a 12.5-μW optical power have been enhanced from 13.7 to 20.2 (88 to 129 μA) due to an emitter-induced gain high (EIGH) from photocurrent modulation. For DEPTs as an electrooptical switch, the EIGH from photocurrent modulation and the emitter-induced gain effect from junction-voltage modulation dominate the dynamic operation. In the case of continuous light input, good bistable-state output characteristics can be realized with an electrical clock signal. When the switch is operated with a 2-V supply voltage and a 10-kΩ load resistance, the stable electrical-logic swing (ELS) is 0.41 V for a 1-V/1-kHz clock signal. Electrical inputs of 5-, 10-, and 50-kHz clock signals are also employed to achieve outputs with increased ELSs of 1.18, 1.19, and 1.3 V, respectively. An optical inverter is realized. When two clock signals, an electrical input and an optical input, are employed, DEPTs are operated as a tristable-state switch. [ABSTRACT FROM AUTHOR]

Fabrication, characterization, and modeling of three-terminal (3T) heterojunction phototransistors (HPTs) using an InGaP layer for passivation (called P-HPTs) compared with similar nonpassivated devices (called NP-HPTs) were reported. Effects of the base passivated by the InGaP layer on devices optical and electrical performance were investigated. In addition to improving the dc current gain in the small current regime, the photocurrent (Iph) and responsivity from the p-i-n diode formed by the base, collector, and subcollector are also enhanced in a P-HPT. The measured optical gains are 45 and 27 for a P- and an NP-HPT under 8.62-μW optical injection operated as a two-terminal (2T) device with a floating base. When the base bias is applied from a voltage source, both 3T P- and NP-HPTs exhibit degraded optical gains. Although a voltage source applied to the base can be used to push the operating point of a heteroj unction bipolar transistor to a higher collector current where the current gain is higher, only a small portion of the photocurrent generated within the base-collector region is injected across the base-emitter junction to be amplified. When the base of an HPT is biased using a current source, the Iph and enhanced dc current gain mainly determine both collector photocurrent and optical gain. Thus, a P-HPT biased using a current source shows the best optical performance. Furthermore, the conventional Ebers-Moll equivalent-circuit model was extended to provide simulated results in good agreement with experiment. [ABSTRACT FROM AUTHOR]