Deposition of Highly Ordered CF
2
-Rich Films Using
Continuous Wave and Pulsed Hexafluoropropylene
Oxide Plasmas
Carmen I. Butoi, Neil M. Mackie, Lara J. Gamble,
†
David G. Castner,
†
Jeffrey Barnd, Anne M. Miller, and Ellen R. Fisher*
Department of Chemistry, Colorado State University, Fort Collins, Colorado 80523-1872
Received March 20, 2000. Revised Manuscript Received May 15, 2000
The structure and composition of fluorocarbon materials deposited in pulsed and continuous
wave (CW) hexafluoropropylene oxide (HFPO) plasmas were investigated. Results indicate
substantial dependence on substrate position relative to the rf coil. When the substrate was
placed 8 cm downstream from the rf coil (25 W CW), highly amorphous, cross-linked films
were obtained. In contrast, materials deposited 28 cm downstream from the rf coil contained
less cross-linked moieties and a higher degree of order. Angle-resolved X-ray photoelectron
spectroscopy (XPS) C
1s
analysis showed that the 28 cm materials contain up to ∼80% CF
2
and CF
3
surface-enriched layers. Static secondary ion mass spectroscopy (SIMS) data revealed
that these fluorocarbon materials are composed of long CF
2
chains. Near edge X-ray
absorption fine structure (NEXAFS) analysis showed that the CF
2
chains were oriented
perpendicular to the substrate surface for the films deposited at 28 cm downstream, while
the films obtained 8 cm downstream do not exhibit any particular orientation. The
compositions of materials deposited in pulsed HFPO systems have rf power and distance
dependencies similar to those observed in the CW plasmas.
I. Introduction
Over the past 20 years, pulsed rf plasmas have been
successfully employed in plasma polymerization of a
variety of monomers.
1,2,3
With pulsed plasma polymer-
ization, high retention of the monomer functional group
in the resulting polymeric film can be achieved.
4
In
addition, pulsed plasmas provide access to lower con-
tinuous wave (CW) equivalent powers because the rf
power is on for only a portion of the cycle time. Use of
pulsed sources reduces trapped radicals in the film,
lowers deposition surface temperatures, decreases high-
energy ion bombardment and UV flux to the surface,
and provides greater control over the resulting film
chemistry.
5
In contrast, films deposited from CW plas-
mas are often amorphous polymeric materials with little
resemblance to the original monomer.
6,7
This is partially
because CW plasmas can significantly fragment and
scramble monomer functional groups through complex
recombination and addition reactions.
8
However, ma-
terials generated at very low CW powers have been
shown to retain some monomer functionalities.
9
Alter-
natively, we have previously reported the use of pulsed
rf plasmas to produce a variety of hydrogenated and
fluorinated organic films with a high degree of control-
lability over film composition.
4
Alternatives to pulsed plasma film deposition are
provided by plasma-enhanced chemical vapor deposition
(PECVD) using downstream and remote CW plasmas,
which also decrease energetic species bombardment of
the deposited material. Again, this eliminates undesired
effects usually associated with the use of CW plasmas
and can produce films with unique properties.
10,11,12
Fluorocarbon materials deposited in this manner have
been shown to possess low dielectric constants
13
and
increased biocompatibility.
14,15
O’Kane and Rice re-
ported pronounced composition differences between
films generated at different distances from the rf glow
†
Department of Bioengineering and Chemical Engineering, Uni-
versity of Washington, Box 1750, Seattle, WA 98195-1750.
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2014 Chem. Mater. 2000, 12, 2014-2024
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Published on Web 06/16/2000