F. Goesmann et R. Schmidfetzer, STABILITY OF W AS ELECTRICAL CONTACT ON 6H-SIC - PHASE-RELATIONS AND INTERFACE REACTIONS IN THE TERNARY-SYSTEM W-SI-C, Materials science & engineering. B, Solid-state materials for advanced technology, 34(2-3), 1995, pp. 224-231
In this study the system W-Si-C was investigated under two aspects, me
tallurgical and electrical, in order to understand the formation and t
he properties of W electrical contacts on 6H-SiC. We combined two diff
erent approaches. For the examination of the phase relations in the te
rnary system we prepared bulk diffusion couples of W and monocrystalli
ne SiC which were annealed and investigated using an SEM (secondary el
ectron images, backscattered electron images. energy dispersive X-ray
analysis). Secondly are furnace molten powder samples, annealed at dif
ferent temperatures, were analysed by X-ray diffraction. To investigat
e the electrical properties of a W/SiC junction transmission line cont
act patterns were sputter deposited onto wafer strips. These samples w
ere subjected to similar heal treatments and the current,voltage chara
cteristics were measured with a source measure unit. Individual contac
t resistivities could be evaluated using a special contact geometry. A
s a result we discovered a four-phase equilibrium in the W-Si-C system
at 1400 +/- 100 degrees C: 3W(5)Si(3) + 7SiCr reversible arrow 8WSi(2
) + 7WC. This is in qualitative agreement with thermodynamic calculati
ons. At 1300 degrees C the equilibrium WSi2 + WC exists. At 1000 degre
es C the reaction kinetics are too slow to be detected in a bulk sampl
e. The phase sequence developing in a bulk W:SiC diffusion couple at 1
300 degrees C is W/W5Si3/WC/SiC. W forms ohmic contacts on n-type 6H-S
iC which are stable up to 1000 degrees C for at least several hours. F
rom 1200 degrees C upwards a reaction between W and SiC leads to the f
ormation of tungsten silicides and carbides and hence a deterioration
of the electrical properties. The films disintegrate into small crysta
ls of WC and W5Si3 leading to a large spread of the resistances of the
individual contacts.