1984
DOI: 10.1103/physrevb.30.4713
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Investigation of hydrocarbon-plasma-generated carbon films by electron-energy-loss spectroscopy

Abstract: The bonding in hard, hydrogenated, amorphous carbon films (a-C:H) prepared by plasma decomposition of benzene was investigated by high-resolution electron-energy-loss spectroscopy. In all asgrown films we find that one-third of the carbon atoms are trigonally bonded and two-thirds of the carbon atoms are tetrahedrally bonded. For the trigonally bonded part, the dielectric properties reveal a transformation from polymeric state for samples prepared with low ion energy to a more graphitic state for films prepare… Show more

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Cited by 271 publications
(77 citation statements)
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“…This broad band results from σ +π excitations and is centred around 27.0 eV for samples prepared with wall temperatures of 100 and 80 • C and at a slightly lower energy of ∼25 eV for T wall = 60 • C. These loss features are typical of graphite-like structures, like carbon nanotubes [32][33][34]. Peaks at ∼6 eV are attributed to π -π* collective excitations.…”
Section: Xps Analysismentioning
confidence: 97%
“…This broad band results from σ +π excitations and is centred around 27.0 eV for samples prepared with wall temperatures of 100 and 80 • C and at a slightly lower energy of ∼25 eV for T wall = 60 • C. These loss features are typical of graphite-like structures, like carbon nanotubes [32][33][34]. Peaks at ∼6 eV are attributed to π -π* collective excitations.…”
Section: Xps Analysismentioning
confidence: 97%
“…Infrared spectra of HAC deposited at low temperatures by plasma deposition show that the hydrogen content and bonding can be influenced by thermal and radiative interactions (Ogmen & Duley 1988;Duley 1994). In the laboratory, HAC is found to graphitize on heating (Wada, Gaczi, & Solin 1980;Smith 1984;Fink et al 1984;Grill, Patel, & Meyerson 1990). This occurs in a series of stages on heating to temperatures T ?…”
Section: Introductionmentioning
confidence: 99%
“…Few laboratory based determinations of optical constants of carbon analogs exist for λ < 120 nm. Fink et al (1984) measured the EELS spectra from 300 nm to 40 nm for amorphous carbons. Colangeli et al (1993) measured the spectra of carbon samples down to ∼50 nm through transmission or reflection on a gold-coated quartz window.…”
Section: General Overviewmentioning
confidence: 99%