The performance of n-type HgCdTe mid-wavelength infrared (MWIR) photoconduc
tors has been investigated using two-dimensional (2-D) device modelling. A
comparison has been made between a practical detector structure with planar
contacts on the upper HgCdTe surface, and a structure commonly used in one
-dimensional (1-D) device modelling with end contacts to the photo-absorbin
g slab of semiconductor. This comparison highlights differences in detector
responsivity, and spatial distribution of both the applied electric field
and photogenerated minority carriers. The practical device structure, where
2-D effects are most evident, provided a good fit to experimental results
for frontside-illuminated n-type HgCdTe photoconductive detectors with n(+)
/n blocking contacts without needing to include S, the contact recombinatio
n velocity, which is commonly employed in 1-D models as a fitting parameter
. Instead, only the n(+) doping density (1 x 10(16) cm(-3)) and n(+) doping
region (depth of 3 mu m), were used to account for the partial blocking of
minority carriers by the contact region. In addition, the 2-D model was us
ed to examine the influence of n(+) blocking contact geometry and doping de
nsity on n-type HgCdTe photoconductor responsivity performance. (C) 2000 El
sevier Science B.V. All rights reserved.