Physical Review Letters · 1997 · 44 citations · 9 references
Natural SciencesMaterials SciencePhysicsElectronic MaterialsSemiconductor MaterialsSpectroscopyAb Initio MethodsDefects In Electronic MaterialsOptical Properties Of SemiconductorsRaman SpectroscopySemiconductor DefectsSemiconductor PhysicsAb Initio CalculationsDeep-level DefectsDefect Levels In SemiconductorsImpurity StatesRaman ScatteringRaman SpectraScatteringVibrational Scattering
Formation of bonded dicarbon C-C centers is deduced from the observation of Raman lines at 1742, 1708, and $1674\mathrm{cm}{}^{\ensuremath{-}1}$ in GaAs codoped with ${}^{12}$C and ${}^{13}$C after annealing at 850 \ifmmode^\circ\else\textdegree\fi{}C with concomitant loss of vibrational scattering from ${\mathrm{C}}_{\mathrm{As}}$. The frequencies agree with results of ab initio theory for a C-C split interstitial (deep donor) formed by the trapping of a mobile interstitial C (displaced ${\mathrm{C}}_{\mathrm{As}}$) atom by an undisplaced ${\mathrm{C}}_{\mathrm{As}}$ acceptor. Other mechanisms of carrier loss are inferred since a weaker Raman triplet is detected at 1859, 1824, and $1788\mathrm{cm}{}^{\ensuremath{-}1}$ from a different C-C complex.
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