Abstract

Resonant Raman scattering has been used to study amorphous carbon and polycrystalline diamond films. The incident photon energies were varied over the range 2.2--4.8 eV. In hydrogenated amorphous carbon films containing both ${\mathrm{sp}}^{3}$- and ${\mathrm{sp}}^{2}$-bonded carbon, a high-frequency shift is observed for the main Raman peak with increasing photon energies up to 3.5 eV. This shift is interpreted in terms of scattering from \ensuremath{\pi}-bonded carbon clusters which is resonantly enhanced for photon energies approaching the \ensuremath{\pi}-${\ensuremath{\pi}}^{\mathrm{*}}$ resonance of ${\mathrm{sp}}^{2}$-bonded carbon. In polycrystalline diamond films excitation with photon energies \ensuremath{\ge}3.0 eV enhances the Raman signal from the ${\mathrm{sp}}^{3}$-bonded diamond phase relative to the scattering by ${\mathrm{sp}}^{2}$-bonded carbon and with respect to the underlying broadband luminescence. The Raman band arising from scattering by ${\mathrm{sp}}^{2}$-bonded carbon shows a high-frequency shift with increasing photon energy for energies \ensuremath{\ge}3.0 eV. Possible models for the structure of this ${\mathrm{sp}}^{2}$-bonded carbon phase are discussed on the basis of the present Raman data.

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