The cathodoluminescence (CL) in ZnSe crystals annealed at T=1200 K in
a Bi melt containing an aluminum impurity is investigated. The spectra
are recorded for different excitation levels, temperatures, and detec
tion delay times t(0). As t(0) is increased, the intensity of the oran
ge band at lambda(max)=630 nm (1.968 eV) in the CL spectrum decreases
in comparison to the intensity of the dominant yellow-green band at la
mbda(max)=550 nm (2.254 eV), whose half-width increases in the tempera
ture range 6-120 K and then decreases as the temperature increases fur
ther. It is shown that such behavior of the yellow-green band is cause
d by the competition between two processes: recombination of donor-acc
eptor pairs and of free electrons with holes trapped on accepters. The
former mechanism is dominant at low temperatures, and the latter mech
anism is dominant at high temperatures. At T similar to 120 mK the con
tributions of the two mechanisms to the luminescence are comparable. T
he resultant structureless band then achieves its greatest half-width,
which is dictated by the interaction of the recombining charge carrie
rs with longitudinal-optical and longitudinal-acoustic phonons and wit
h the free-electron plasma. The mean number of longitudinal-optical ph
onons emitted per photon is determined mainly by their interaction wit
h holes trapped on deep accepters in the form of Al atoms replacing Se
. The donor in the pair under consideration is an interstitial Al atom
. (C) 1997 American Institute of Physics.