Application of perturbation theory to finding vibrational frequencies of a spheroid
Authors: M. O. Nestoklon, L. Saviot, S. V. Goupalov
AI-generated Key Points
- Study by Nestoklon, Saviot, and Goupalov explores vibrational frequencies of Raman-active spheroidal modes compared to spheres using perturbation theory of boundary conditions.
- Method developed by Migdal and Moszkowski for deformed atomic nuclei applied to analyze eigenfrequencies of CdSe and silver nanoparticles focusing on $j=2$ angular momentum modes.
- Perturbation method accurately predicts frequency splittings under rigid boundary conditions resembling a sphere's shape closely.
- Limitations arise when dealing with stress-free boundaries in predicting frequency splittings.
- Research offers valuable insights into vibrational frequencies in non-spherical structures and provides comparisons between theoretical predictions and numerical calculations.
Abstract: We apply perturbation theory of boundary conditions, originally developed by A.B. Migdal and independently by S.A. Moszkowski for deformed atomic nuclei, to finding eigenfrequencies of Raman-active spheroidal modes of a spheroid from these of a sphere and compare the outcomes with the results of numerical calculations for CdSe and silver nanoparticles. The modes are characterized by the total angular momentum $j=2$ and are five-fold degenerate for a sphere but split into three distinct modes, characterized by the absolute value of the total angular momentum projection onto the spheroidal axis, in case of a spheroid. The perturbation method works well in case of the rigid boundary conditions, with the displacement field set to zero at the boundary, and accurately predicts the splittings when the spheroidal shape is close to a sphere, but fails in case of the stress-free boundary conditions.
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