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Vibrational Spectra and Structures of Neutral Si<sub><i>m</i></sub>C<sub><i>n</i></sub> Clusters (<i>m</i> + <i>n</i> = 6): Sequential Doping of Silicon Clusters with Carbon Atoms
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Citations
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References
2012
Year
EngineeringChemistrySilicon On InsulatorSemiconductor NanostructuresSemiconductorsNanoelectronicsQuantum MaterialsSiliceneSilicon ClustersCluster ScienceStable IsomersSequential DopingPhysicsInfrared SpectroscopyBare SiPhysical ChemistryQuantum ChemistryVibrational SpectraGas PhaseSpectroscopyNatural SciencesCondensed Matter PhysicsApplied PhysicsCluster ChemistryCarbide
Vibrational spectra of mixed silicon carbide clusters Si(m)C(n) with m + n = 6 in the gas phase are obtained by resonant infrared-vacuum-ultraviolet two-color ionization (IR-UV2CI for n ≤ 2) and density functional theory (DFT) calculations. Si(m)C(n) clusters are produced in a laser vaporization source, in which the silicon plasma reacts with methane. Subsequently, they are irradiated with tunable IR light from an IR free electron laser before they are ionized with UV photons from an F(2) laser. Resonant absorption of one or more IR photons leads to an enhanced ionization efficiency for Si(m)C(n) and provides the size-specific IR spectra. IR spectra measured for Si(6), Si(5)C, and Si(4)C(2) are assigned to their most stable isomers by comparison with calculated linear absorption spectra. The preferred Si(m)C(n) structures with m + n = 6 illustrate the systematic transition from chain-like geometries for bare C(6) to three-dimensional structures for bare Si(6). In contrast to bulk SiC, carbon atom segregation is observed already for the smallest n (n = 2).
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