COMPUTER-SIMULATION OF THE PHOTOLUMINESCENCE DECAY AT THE GAAS ELECTROLYTE JUNCTION .1. THE INFLUENCE OF THE EXCITATION INTENSITY AT THE FLAT-BAND CONDITION
O. Kruger et al., COMPUTER-SIMULATION OF THE PHOTOLUMINESCENCE DECAY AT THE GAAS ELECTROLYTE JUNCTION .1. THE INFLUENCE OF THE EXCITATION INTENSITY AT THE FLAT-BAND CONDITION, Journal of physical chemistry, 98(48), 1994, pp. 12653-12662
The influence of excitation intensity, surface recombination velocity,
and photocurrent on the time-resolved photoluminescence (PL) at the n
-GaAs-electrolyte junction under flat band conditions was investigated
using computer simulations. The mathematical background of the two-di
mensional semiconductor analysis package (TOSCA) will be presented. We
will show that the effects may be characterized qualitatively by expo
nential fit function(s), although in most cases the simulated PL decay
is nonexponential. For a free carrier concentration n(0) = 5 x 10(17)
cm(-3), under the conditions of low injection density (p(i)) and with
flat bands, both the surface recombination and the photocurrent lead
to a remarkable decrease in the FL decay time either for surface recom
bination velocities S-0 > 10(3) cm/s or for exchange photocurrent dens
ities j(ph,0) > 10(-11) A/cm(2). Under the conditions chosen in this w
ork, the PL decay time approximated by the monoexponential decay time
T decreases to a minimum value in T-min = 1.64 ns when S-0 greater tha
n or equal to 10(6) cm/s or j(ph,0) > 10(-8) A/cm(2). This minimum ind
icates that the diffusion of the minority carriers toward the surface
where they immediately nonradiatively vanish by means of surface recom
bination and/or charge transfer, respectively, is limited by the therm
al velocity. In both cases, diffusion competes effectively against bul
k recombination. For injection levels (p(i)/n(0)) > 0.1, the PL decay
time decreases with increasing injection density because the quadratic
recombination process dominates. At high injection densities, the sur
face recombination velocity may not remain constant during the PL deca
y, but instead varies as a function of time S(t); S may decrease from
its maximum value (S-0) by up to 1 order of magnitude during the PL de
cay. The results will be discussed in relation to experimental results
published previously by other groups.