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<p>Amorphous
boron-carbon-nitrogen (B-C-N) films with low density are potentially
interesting as alternative low-dielectric-constant (low-κ) materials for future
electronic devices. Such applications require deposition at temperatures below
300 °C, making plasma chemical vapor deposition (plasma CVD) a preferred
deposition method. Plasma CVD of B-C-N films is today typically done with
separate precursors for B, C and N or with precursors containing B–N bonds and
an additional carbon precursor. We present an approach to plasma CVD of B-C-N
films based on triethylboron (B(C<sub>2</sub>H<sub>5</sub>)<sub>3</sub>) a
precursor with B-C bonds in an argon-nitrogen plasma. From quantitative
analysis with Time-of-Flight Elastic Recoil Detection Analysis (ToF-ERDA), we
find that the deposition process can afford B-C-N films with a B/N ratio
between 0.98 and 1.3 and B/C ratios between 3.4 and 8.6 and where the films
contain between 3.6 and 7.8 at. % H and 6.6 and 20 at. % of O. The films have
low density, from 0.32 to 1.6 g/cm<sup>3</sup> as determined from cross-section
scanning electron micrographs and ToF-ERDA
with morphologies ranging from smooth films to separated nanowalls. Scaning
transmission electron microscopy shows that C and BN does not phase seperarte
in the film. The static dielectric constant κ, measured by capacitance–voltage
measurements<b>,</b> varies with the Ar concentration in the range from 3.3 to
35 for low and high Ar concentrations, respectively. We
suggest that this dependence is caused by the energetic bombardment of plasma species during film deposition.</p>
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