2005
DOI: 10.1103/physrevb.72.205433
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Longitudinal versus transverse spheroidal vibrational modes of an elastic sphere

Abstract: Analysis of the spheroidal modes of vibration of a free continuum elastic sphere show that they can be qualitatively grouped into two categories: primarily longitudinal and primarily transverse. This is not a sharp distinction. However, there is a relatively stark contrast between the two kinds of modes. Primarily transverse modes have a small divergence and have frequencies that are almost functionally independent of the longitudinal speed of sound. Analysis of inelastic light scattering intensity from confin… Show more

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Cited by 41 publications
(33 citation statements)
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“…25 They also showed that modes of both natures are present in a sequence ͑n , l͒ with fixed l Ͼ 0, whereas for l = 0, all modes have a dominant longitudinal character. The longitudinal or transverse nature of a mode will determine its contribution to the VV Raman and Brillouin terms or to the HV Raman term, respectively.…”
Section: ͑19͒mentioning
confidence: 97%
“…25 They also showed that modes of both natures are present in a sequence ͑n , l͒ with fixed l Ͼ 0, whereas for l = 0, all modes have a dominant longitudinal character. The longitudinal or transverse nature of a mode will determine its contribution to the VV Raman and Brillouin terms or to the HV Raman term, respectively.…”
Section: ͑19͒mentioning
confidence: 97%
“…4 In order to confirm the validity of this simple approach for spherical nanoparticles, we use a method similar to the one used in a previous work. 17 Studying the frequency changes resulting from a continuous variation of the elasticity of the material the sphere is made of provides some insight into the nature of the vibrations. A cubic material has three independent elastic constants C 11 , C 12 and C 44 instead of two for isotropic elasticity for which C 44 = C11−C12…”
Section: Methodsmentioning
confidence: 99%
“…The lowest energy mode, however, belongs to a set of l ¼ 2 solutions (in the simplest of which, the sphere is deformed to an oblate, then to a prolate spheroid [15]), and has an energy of approximately 40% of that of the l ¼ 0 mode (for a more detailed solution see, for example, Salvador et al [16]). Regardless of the details of the mode, Lamb theory solutions are characterized by a 1=r dependence of the discrete acoustic-phonon energy on the particle radius.…”
mentioning
confidence: 99%