Electrodeposited, dc magnetron sputtered, and electron beam evaporated Pt c
ontacts to n-GaN (n=1.5x10(17) cm(-3)) are reported. All contacts were rect
ifying in the as-deposited condition, and values of the barrier height were
determined by current-voltage (I-V) and capacitance-voltage (C-V) measurem
ents. The influence of deposition conditions on the electrical characterist
ics of the sputtered and electrodeposited Pt contacts was further studied.
Additionally, a dependence of the barrier height with time following deposi
tion is shown. Taking into consideration all parameters of this study, the
barrier height could differ by as much as 0.65 eV by I-V measurements and 0
.64 eV by C-V measurements, with I-V and C-V barriers as high as 1.43 and 1
.57 eV, respectively. Reverse current densities are reported for a -5 V bia
s with the highest and lowest median values differing by a factor of 10(4)
as a result of the different deposition conditions. The electrical properti
es are believed to be strongly influenced by the presence of electrically a
ctive defects introduced during metal deposition. Deep level transient spec
troscopy data support this hypothesis. (C) 2000 American Institute of Physi
cs. [S0021-8979(00)07417-X].