C-ENERGY-DEPENDENT RESIDUAL ION DAMAGE IN GAAS-C GROWN BY THE LOW-ENERGY ION-BEAM DOPING METHOD()
Citation
T. Iida et al., C-ENERGY-DEPENDENT RESIDUAL ION DAMAGE IN GAAS-C GROWN BY THE LOW-ENERGY ION-BEAM DOPING METHOD(), Journal of applied physics, 80(7), 1996, pp. 3828-3833
Categorie Soggetti
Physics, Applied
SICI code
0021-8979(1996)80:7<3828:CRIDIG>2.0.ZU;2-#
Abstract
The effects of residual ion damage in low-energy (30 eV-30 keV) C+-dop
ed GaAs investigated with regard to the electrical and optical activat
ion of C as a function of C+ ion acceleration energy ECL. Systematic v
ariation of E(C+) demonstrated that, in the energy range of E(C+) < 17
0 eV, the net hole concentration (\N-A-N-D\) slightly increases as E(C
+) increase sand the highest \N-A-N-D\ was obtained al E(C+) = 170 eV
under the constant C+ ion-beam current density. For E(C+) > 170 eV. an
increase in E(C+) gave rise to an abrupt decrease of \N-A-N-D\ down t
o two orders of magnitude smaller than that obtained al E(C+) 170 eV,
Ln Low-temperature (2 K) photoluminescence spectra for as-grown sample
s with E(C+) = 240 and 350 eV, a novel emission ascribable to residual
ion damage was observed instead of an essential acceptor-acceptor emi
ssion of [g-g](beta). However, subsequent annealing at 850 degrees C m
ade this novel emission disappear and the proper [g-g](beta) emission
was merely observed. An activation process observed for E(C+) = 5, 10,
and 30 keV samples was very similar to that by high-energy ion implan
tation, indicating low activation rate of 10%-15%. Minority-carrier li
fetime measurements using scanning tunneling microscope stimulated lim
e-resolved luminescence demonstrated the presence of residual ion dama
ge in as-grown samples at E(C+) = 240 and 350 eV and annealed ones at
E(C+) = 5, 10, and 30 keV while no ion damage was observed in as-grown
sample at E(C+) = 30 eV, The incorporation and activation behaviors o
f C atoms that take the Term of low-energy ions were found to be consi
derably affected by changes in ion-surface interaction with increasing
E(C+) and by the presence of residual ion damage in the layer. (C) 19
96 American Institute of Physics.