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Electronic Material Properties - und Geowissenschaften ...

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Figure 2 shows the successful coating of plasma polymerized hexafluoro-m-xylene<br />

on ZrO2. Polymerization through plasma agitation always leads to an amorphous<br />

coating that can be clearly distinguished from the dark and crystalline oxide core. In<br />

all cases, oxide particles can be produced with diameters smaller than 10 nm and<br />

varying coating thickness of 2 - 10 nm.<br />

Fig. 2: Transmission electron micrograph of<br />

an amorphous polymer coating on the zirconia<br />

core (Image by R. Schierholz, Structural<br />

research division).<br />

Transmittance T [a.u.]<br />

3180<br />

ν (N-H)<br />

ν (C-H)<br />

ppECA/<br />

SiO (p)<br />

2<br />

CO<br />

2<br />

ppMMA/<br />

SiO 2<br />

SiO 2<br />

1600<br />

ν<br />

1710<br />

(C=C)<br />

ν (-C=O)<br />

δ (C-H)<br />

880<br />

δ (Si(CH 3 ) 2 )<br />

3000 2000 1000<br />

Wavenumber [cm -1 ]<br />

*<br />

*<br />

*<br />

* SiO 2<br />

*<br />

*<br />

*<br />

664<br />

δ (N-H 2 )<br />

Fig. 3: FT-IR spectra of uncoated silica, silica<br />

coated with plasma polymerized MMA<br />

(ppMMA/SiO2) and silica coated with plasma<br />

polymerized ECA (ppECA/SiO2).<br />

The influence of the coating material on the dispersability was studied in the case of<br />

the acrylate-based coatings ppMMA and ppECA on silica [3] . Powders derived from<br />

methylmethacrylate are characterised by a hydrophobic surface, making it impossible<br />

to disperse them in water. The powders are not wettable. The exchange of a methyl<br />

group to a cyano group (-CN) in the monomer leads to enhanced dispersability in<br />

water. In the plasma, the C≡N bond is split and reassembled with hydrogen in the<br />

coating to form –NH2 groups, as determined by FT-IR spectroscopy (Fig. 3). The<br />

hydrocarbon bands of the coating can be fo<strong>und</strong> in the range of 2875 – 2960 cm -1 .<br />

Vibrations of the methacrylate can be identified aro<strong>und</strong> 1710 cm -1 for the C=O bond<br />

and aro<strong>und</strong> 1600 cm -1 for the double bonded carbon. The vibrations responsible for<br />

δ(N-H2) aro<strong>und</strong> 664 cm -1 and for ν(N-H) aro<strong>und</strong> 3180 cm -1 appear only in the<br />

spectrum measured on particles coated with ECA-derived coatings.<br />

Literatur:<br />

[1] J. Suffner, Diploma thesis, Faculty of <strong>Material</strong>s- and Geo-Sciences (TU<br />

Darmstadt), 2006<br />

[2] M. Schallehn, M. Winterer, T.E. Weidrich, U. Keiderling, H. Hahn, Chem. Vap.<br />

Deposition 2001, 9, 40.<br />

[3] J. Suffner, G. Schechner, H. Sieger, H. Hahn, Chem. Vap. Deposition<br />

(accepted for publication)<br />

- 109 -<br />

*<br />

*<br />

*

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