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Copyright © 2007 American Scientific Publishers
All rights reserved
Printed in the United States of America
Journal of
Nanoscience and Nanotechnology
Vol. 7, 2192–2196, 2007
PreferredOrientationinRuNanocolumns
InducedbyResidualOxygen
J. P. Singh
1 ∗
, T. Karabacak
2
, P. Morrow
2
, S. Pimanpang
2
, T.-M. Lu
2
, and G.-C. Wang
2
1
Physics Department, Indian Institute of Technology Delhi, Hauz Khas, New Delhi 110016, India
2
Department of Physics, Applied Physics and Astronomy Rensselaer Polytechnic Institute,
Troy, New York 12180-3590, USA
Ru nanocolumns were grown on a native oxide covered Si(100) substrate using an oblique angle
sputter deposition technique with substrate rotation at room temperature. Scanning tunneling
microscopy images of conventional Ru film show the presence of straight columnar features on the
film surface, which are very different from the nearly circular features observed on the nanocolumns
surface. X-ray diffraction spectra confirm that these nanocolumns have (100) as the preferred ori-
entation instead of the (002) orientation observed for a conventional film. The oxygen to Ru atomic
ratio was determined for both the nanocolumns and the conventional film by using X-ray photo-
electron spectroscopy. The nanocolumns were observed to incorporate about 6 times more oxygen
than the conventional film near the surface region. We argue that the oxygen segregates onto the
high-density (002) plane whereas it permeates through comparatively open planes like (100) and
(101). The adsorbed oxygen atoms serve as a diffusion barrier for the landing Ru adatoms and
inhibit the growth of the (002) plane. This results in the absence of the (002) plane and development
of (100) and (101) planes in the nanocolumns. The oxygen plays a decisive role in determining the
crystallographic orientation and the feature size/shape over the nanocolumns and conventional film
surfaces.
Keywords: Ruthenium, Oblique Angle Deposition, dc Magnetron Sputtering, Scanning Tunneling
Microscopy, X-ray Photoelectron Spectroscopy.
1. INTRODUCTION
Crystalline Ruthenium (Ru) is a noble metal with a hexag-
onal close packed (hcp) structure. Among various con-
tact electrodes, Ru is rather appealing for microelectronic
applications because its oxide serves as a barrier to diffu-
sion, but is electrically conducting.
1–2
Another application
of Ru is in the capacitor electrodes.
3
An understanding
of the detailed structure and surface morphology of Ru
nanowires
4
is of great importance for nanoscale inter-
connect technology.
In general, during the growth of a polycrystalline film,
the crystallographic axis is aligned along a preferred direc-
tion but the orientation is random in the plane of the sub-
strate. The preferred direction is normal to the substrate
with the densest crystallographic planes parallel to the sub-
strate, for example, the (111), (110), and (001) planes for
the fcc, bcc, and hcp crystals, respectively.
5
The initial ori-
entation is driven by the crystal’s tendency to approach a
minimum surface energy configuration, but the final pre-
ferred orientation is influenced by various factors such as
∗
Author to whom correspondence should be addressed.
substrate temperature, vapor flux direction, sticking coef-
ficient, re-emission, surface diffusion of landing atoms on
the substrate, and residual gas in the vacuum chamber. For
example, the (111) texture for sputtered Cu films has been
observed to change to the (100) texture after 40 hours
at room temperature.
6
In addition, oxygen induced pre-
ferred orientation has been observed in many metals.
7 8
For example, the orientation of Pt film deposited on a glass
substrate can be changed from the (111) to the (200) with
the presence of oxygen during the deposition.
7
In this letter, we show that the Ru nanocolumns have
the (100) preferred orientation instead of the (002) orien-
tation observed for a conventional film. These Ru nano-
columns were grown by an oblique angle deposition
(OAD) technique.
9–10
The OAD allows a single step fab-
rication of nanocolumns and other desired geometries. It
is a physical vapor deposition in which flux arrives at a
large oblique incidence angle (>80
) from the substrate
normal while the substrate is rotating. This results in the
formation of isolated nanocolumns by the self-shadowing
mechanisms. Our Ru nanocolumns were deposited on
native oxide covered p-Si(100) (resistivity 12–25 -cm)
2192 J. Nanosci. Nanotechnol. 2007, Vol. 7, No. 6 1533-4880/2007/7/2192/005 doi:10.1166/jnn.2007.793