The epitaxial growth of HgCdTe on alternative substrates has emerged as an
enabling technology for the fabrication of large-area infrared (IR) focal p
lane arrays (FPAs). One key technical issue is high dislocation densities i
n HgCdTe epilayers grown on alternative substrates. This is particularly im
portant with regards to the growth of HgCdTe on heteroepitaxial Si-based su
bstrates, which have a higher dislocation density than the bulk CdZnTe subs
trates typically used for epitaxial HgCdTe material growth. In the paper a
simple model of dislocations as cylindrical regions confined by surfaces wi
th definite surface recombination is proposed. Both radius of dislocations
and its surface recombination velocity are determined by comparison of theo
retical predictions with carrier lifetime experimental data described by ot
her authors. It is observed that the carrier lifetime depends strongly on r
ecombination velocity; whereas the dependence of the carrier lifetime on di
slocation core radius is weaker. The minority carrier lifetime is approxima
tely inversely proportional to the dislocation density for densities higher
than 10(5) cm(-2). Below this value, the minority carrier lifetime does no
t change with dislocation density. The influence of dislocation density on
the R(o)A product of long wavelength infrared (LWIR) HgCdTe photodiodes is
also discussed. It is also shown that parameters of dislocations have a str
ong effect on the R(o)A product at temperature around 77 K in the range of
dislocation density above 10(6) cm(-2). The quantum efficiency is not a str
ong function of dislocation density.