2003
DOI: 10.1016/s0925-9635(02)00222-4
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Dielectric function, electronic properties and optical constants of amorphous carbon and carbon nitride films

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Cited by 54 publications
(42 citation statements)
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“…The resonance energy for π→π* electronic transitions for crystalline graphite is found at 4.5 eV but the energy decreases when the amount of sp 2 -clusters in the matrix increases [36] or when the sp 2 sites exhibit a different arrangement [19]. This is in agreement with the lower resonance energies noticed for these films, located between 31000-32450 cm -1 (3.8 and 4.0 eV), where the lowest energy is observed for the g-CN x film (G8) and the highest for the FL-CN x film (F9) [19,37]. The strongest peak for the π→π* transition is noticed for the a-C film (C8) [19] and the weakest for the FL-CN x film, which might be explained by a higher disorder in the sp 2 matrix for the FL and graphitic films which reduces the conjugation of the π electrons [13].…”
Section: Range 31000-32450 CM -1 (38-40 Ev) → *supporting
confidence: 84%
“…The resonance energy for π→π* electronic transitions for crystalline graphite is found at 4.5 eV but the energy decreases when the amount of sp 2 -clusters in the matrix increases [36] or when the sp 2 sites exhibit a different arrangement [19]. This is in agreement with the lower resonance energies noticed for these films, located between 31000-32450 cm -1 (3.8 and 4.0 eV), where the lowest energy is observed for the g-CN x film (G8) and the highest for the FL-CN x film (F9) [19,37]. The strongest peak for the π→π* transition is noticed for the a-C film (C8) [19] and the weakest for the FL-CN x film, which might be explained by a higher disorder in the sp 2 matrix for the FL and graphitic films which reduces the conjugation of the π electrons [13].…”
Section: Range 31000-32450 CM -1 (38-40 Ev) → *supporting
confidence: 84%
“…The TL dispersion model is also widely used for modelling the optical dispersion of a-C, a-C: H [44] as well as polycrystalline diamond films [45]. The model is a combination of the Tauc joint density of states [42] and the quantum-mechanical Lorentz oscillator model [46]. The TL model fits to the dielectric functions of a class of an amorphous material.…”
Section: Spectroscopic Ellipsometry Measurement Systemmentioning
confidence: 99%
“…Such approach has been recently applied by Zimmer et al [42] for boron-doped NCD films, Hu et al [15] for MCD films, and Jellison et al [43] for amorphous semiconductors. The model is a combination of the Tauc joint density of states [44] and the quantum mechanical Lorentz oscillator model [45]. The TL model fits to the dielectric functions of a class of amorphous materials.…”
Section: Diamond Growth On Fibresmentioning
confidence: 99%