energetically favorable sites and form diamond nuclei. Al-
though heterogeneous nucleation of diamond on a solid sur-
face from the gas phase is not well understood it has been
demonstrated that diamond readily nucleates on biased
-SiC.1
1,12
A surface layer which consists of a mixture of

amorphous SiC and microcrystalline SiC is seen to form on
Si during biasing.1 These SiC microcrystallites could serve
as nucleation sites for diamond. Similarly, crystallites in the
,13
SiC surface layer formed on SiO surfaces during biasing
2
might act as diamond nucleation sites. A difference in crys-
tallinity or morphology of the SiC overlayers could explain
the lower diamond nucleation densities induced by BEN ob-
8
2
served in this study on SiO ͑ϳ10 /cm ͒ compared to those
2
11
2
1
commonly reported for nucleation on Si (10 /cm ). The
crystallinity of the SiC surface layer formed on an amor-
phous SiO surface would be expected to be lower than that
2
of the SiC layer formed on single-crystal Si surfaces. Thus it
may be possible to increase the nucleation density of dia-
mond produced on SiO via BEN by optimizing process con-
2
ditions to increase the crystallinity of the carbide surface
layer formed.
Bias-enhanced nucleation has been demonstrated to be a
viable in situ process for deposition of diamond on SiO2;
however, more work is required to develop this technique for
production of thinner, smoother diamond films that could be
of use in fabrication of microelectronic devices or optical
coatings. An investigation is currently underway in which
bias-pretreated SiO surfaces will be more thoroughly char-
2
acterized and process conditions used during the pretreat-
ment will be optimized in order to increase the density of
nuclei produced by biasing.
1
B. R. Stoner, G.-H. M. Ma, S. D. Wolter, and J. T. Glass, Phys. Rev. B 45,
1
1067 ͑1992͒.
2
3
P. Reinke, P. Kania, and P. Oelhafen, Thin Solid Films 270, 124 ͑1995͒.
S. D. Wolter, M. T. McClure, J. T. Glass, and B. R. Stoner, Appl. Phys.
Lett. 66, 2810 ͑1995͒.
S. D. Wolter and J. T. Glass, J. Appl. Phys. 77, 5199 ͑1995͒.
J.-S. Lee, K.-S. Liu, and I.-N. Lin, J. Appl. Phys. 81, 486 ͑1997͒.
S. D. Wolter, T. H. Borst, A. Vescan, and E. Kohn, Appl. Phys. Lett. 68,
4
5
6
3
558 ͑1996͒.
7
C. Wild, P. Koidl, W. M u¨ ller-Sebert, H. Walcher, R. Kohl, N. Herres, R.
Locher, R. Samlenski, and R. Brenn, Diam. Relat. Mater. 2, 158 ͑1993͒.
S. Yugo, T. Kimura, and T. Kanai, Diam. Relat. Mater. 2, 328 ͑1992͒.
S. P. McGinnis, M. A. Kelly, and S. B. Hagstr o¨ m, Appl. Phys. Lett. 66,
FIG. 4. ͑a͒ Silicon 2p and ͑b͒ carbon 1s x-ray photoelectron spectra taken
after a 30 min bias pretreatment.
8
9
3
117 ͑1995͒.
1
1
1
0
1
2
J. Gerber, S. Sattel, K. Jung, H. Ehrhardt, and J. Robertson, Diam. Relat.
Mater. 4, 559 ͑1995͒.
B. R. Stoner, G. H. Ma, S. D. Wolter, W. Zhu, Y.-C. Wang, R. F. Davis,
and J. T. Glass, Diam. Relat. Mater. 2, 142 ͑1993͒.
R. Kohl, C. Wild, N. Herres, P. Koidl, B. R. Stoner, and J. T. Glass, Appl.
Phys. Lett. 63, 1792 ͑1993͒.
Diamond may subsequently nucleate on the silicon carbide
or other carbonaceous species present on this surface layer.
It is generally accepted that one primary effect of the
applied bias is to increase the flux of positively charged radi-
ϩ
ϩ
8–10
cals such as C and CH to the substrate surface.
These
13
J. Gerber, S. Sattel, H. Ehrhardt, J. Robertson, P. Wurzinger, and P. Pon-
gratz, J. Appl. Phys. 79, 4388 ͑1996͒.
radicals may react with, or attach to, the substrate surface at
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18 Appl. Phys. Lett., Vol. 71, No. 5, 4 August 1997 Irwin et al.
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