The traditional substrate of choice for HgCdTe material growth has been lat
tice matched bulk CdZnTe material. However, as larger array sizes are requi
red for future devices, it is evident that current size limitations of bulk
substrates will become an issue and therefore large area Si substrates wil
l become a requirement for HgCdTe growth in order to maintain the cost-effi
ciency of future systems. As a result, traditional substrate mounting metho
ds that use chemical compounds to adhere the substrate to the substrate hol
der may pose significant technical challenges to the growth and fabrication
of HgCdTe on large area Si substrates. For these reasons, non-contact (ind
ium-free) substrate mounting was used to grow mid-wave infrared (MWIR) HgCd
Te material on 3" CdTe/Si substrates. In order to maintain a constant epila
yer temperature during HgCdTe nucleation, reflection high-energy electron d
iffraction (RHEED) was implemented to develop a substrate temperature rampi
ng profile for HgCdTe nucleation. The layers were characterized ex-situ usi
ng Fourier transform infrared (FTIR) and etch pit density measurements to d
etermine structural characteristics. Dislocation densities typically measur
ed in the 9 x 10(6) cm(-2) to 1 x 10(7) cm(-2) range and showed a strong co
rrelation between ramping profile and Cd composition, indicating the unique
ness of the ramping profiles. Hall and photoconductive decay measurements w
ere used to characterize the electrical properties of the layers. Additiona
lly, both single element and 32 x 32 photovoltaic devices were fabricated f
rom these layers. A RA value of 1.8 x 10(6) Omega -cm(2) measured at - 40 m
V was obtained for MWIR material, which is comparable to HgCdTe grown on bu
lk CdZnTe substrates.