Quantification of Fluorine Density in the Outermost
Atomic Layer
R. D. van de Grampel,
†,§
W. Ming,*
,†
A. Gildenpfennig,
‡
J. Laven,
†
H. H. Brongersma,
‡
G. de With,
†
and R. van der Linde
†
Laboratory of Coatings Technology, Eindhoven University of Technology, P.O. Box 513,
5600 MB Eindhoven, The Netherlands, and Calipso BV, P.O. Box 513,
5600 MB Eindhoven, The Netherlands
Received July 18, 2003
The outermost atomic layer of perfluorinated thiol monolayers on gold and poly(tetrafluoroethylene)
(PTFE) is analyzed by low-energy ion scattering. Absolute quantification of fluorine density in this layer
was achieved after calibrating the fluorine signal with a freshly cleaved LiF(100) single crystal. The
fluorine density of monolayers of a C8F17-thiol on gold was 1.48 × 10
15
F atoms/cm
2
, whereas for PTFE
a value of 1.24 × 10
15
F atoms/cm
2
was observed. This difference was explained by the different tilt angles
of the thiol on gold and PTFE chains with respect to the surface normal. Both a configurational and a
molecular interpretation on the perfluorinated thiol monolayer on gold are given.
1. Introduction
1.1. General. The surface of materials often plays a
central role for their applications. Understanding of the
physical and chemical properties of surfaces is of para-
mount importance for the design of novel materials.
Fluorinated polymers belong to a class of materials with
exceptional properties. These properties originate from
the nature of the carbon-fluorine bond and the orientation
of the fluorinated tail. From both a fundamental and an
application point of view, it is desirable to gain control
over the wetting properties of fluorinated materials.
Modern surface analytical methods such as X-ray pho-
toelectron spectroscopy (XPS),
1
time-of-flight secondary
ion mass spectroscopy (TOF-SIMS),
2
atomic force micros-
copy (AFM),
3
scanning force microscopy (SFM),
4
and near-
edge X-ray absorption fine structure (NEXAFS)
5
have been
used to elucidate many aspects of the chemical composition
as well as the structure of fluorinated surfaces. These
methods provide useful information on the spatial varia-
tion in chemical composition near the surfaces. But none
of them can exclusively analyze the composition of the
outermost atomic layer.
Nevertheless, from the nature of the forces involved,
for example, van der Waals interactions, it is expected
that the outermost atomic layer of the surface predomi-
nantly determines the wettability. Consequently, the
wettability of an organic material is not related to the
overall chemical composition but rather depends on the
chemical nature of the outermost functional groups.
Zisman
6
observed that the surface free energy decreases
depending on the chemical composition of the material in
the sequence -CH
2
->-CH
3
>-CF
2
->-CF
3
. There-
fore, knowledge of the interfacial behavior (e.g., surface
energies) in relation to surface composition will contribute
to a better understanding and prediction of adhesion and
wetting phenomena. This means that characterization of
the chemical composition of the outermost atomic layer is
highly relevant. Low-energy ion scattering (LEIS), also
referred to as ion scattering spectroscopy (ISS), is a unique
technique that exclusively probes the first atomic layer
of the surface (even when the sample surface is not
smooth).
7
1.2. LEIS. In a LEIS experiment, the sample is bom-
barded with low-energy noble gas ions. The energy of the
ions that are elastically backscattered provides direct
information on the masses of the atoms from which the
ions are scattered. Such an ion scattering experiment is
similar to a “billiard ball” collision; that is, energy and
momentum are conserved in a collision. LEIS is a surface
technique sensitive to the outermost atomic layer only.
8
This is due to the fact that primary ions that collide with
sample atoms have a high probability to capture an
electron leading to neutralization. For ions that penetrate
beyond the first atomic layer, the interaction time is so
long that all ions will be effectively neutralized. Since
electrostatic deflection is used in the analyzer, neutral
species are not detected. This results in a negligible scat-
tered-ion yield from atoms below the first atomic layer.
* To whom correspondence should be addressed. Fax: +31-40-
2445619. E-mail: w.ming@tue.nl.
†
Eindhoven University of Technology.
‡
Calipso BV.
§
Current address: General Electric Plastics, P.O. Box 117, 4600
AC Bergen op Zoom, The Netherlands. E-mail: robert.vandegrampel@
gepex.ge.com.
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10.1021/la0353071 CCC: $27.50 © 2004 American Chemical Society
Published on Web 11/18/2003