CATHODOLUMINESCENCE AND ELECTRON-BEAM-INDUCED CURRENT STUDY OF PARTIALLY RELAXED ALGAAS GAAS/INGAAS HETEROJUNCTION PHOTOTRANSISTORS UNDER OPERATING-CONDITIONS/
O. Sjolund et al., CATHODOLUMINESCENCE AND ELECTRON-BEAM-INDUCED CURRENT STUDY OF PARTIALLY RELAXED ALGAAS GAAS/INGAAS HETEROJUNCTION PHOTOTRANSISTORS UNDER OPERATING-CONDITIONS/, Journal of applied physics, 82(3), 1997, pp. 1438-1445
We have studied time-resolved cathodoluminescence (CL) and electron be
am induced current (EBIC) on AlGaAs/GaAs/InGaAs heterojunction phototr
ansistors under operating conditions, i.e., at room temperature and un
der bias. Devices from four wafers, with a different amount of lattice
relaxation, were tested, It is shown that the CL intensity increases
more than one order of magnitude as the voltage is Increased and the c
urrent gain of the device turns on. The voltage dependence of the CL s
ignal is analogous to the current-voltage curve of the transistor, The
buildup in CL intensity was found to be much less in devices with low
current gain showing that the CL intensity correlates to the electric
al gain of the device. Time resolved CL showed two distinct CL decay t
imes, one very short, a few nanoseconds, and one long, of the order of
microseconds. This indicates that two fundamental recombination proce
sses are present, which we attribute to a spatially direct recombinati
on between carriers in the base and a spatially indirect recombination
. This spatially indirect recombination is believed to come from recom
bination of electrons trapped in the notch formed at the conduction ba
nd discontinuity and holes in the base. By studying EBIC as a function
of beam current for devices from the different wafers we found that r
elaxed devices have a complex current-gain relationship. They require
higher current densities than nonrelaxed devices to reach high gain, A
t low current densities the gain is very low and the ideality factor i
s high indicating a high degree of trap related recombination. At high
current densities, on the other hand, these traps become filled and t
he associated recombination quenched. This results in a gain and an id
eality factor comparable to those of nonrelaxed devices. (C) 1997 Amer
ican Institute of Physics.