“…The calculation for homogeneous spheres can be found in literature [53] as well as the solutions for inhomogeneous core-shell particles. [76] Coming back to our system with N scatterers, the total wave field incident on the n-th scatterer is the sum of the incident plane wave and the wave field scattered from all scatterers n ′ = n.…”
Section: The Multiple Scattering Methodsmentioning
confidence: 99%
“…[40,76,80] For a slab parallel to a distinct crystallographic plane, the reduced vector parallel to this plane, k , is usually a conserved quantity. Therefore, LMS searches in each individual slab propagating Bloch waves for given ω and k , which are the eigenmodes of the elastic field in that slab.…”
Section: The Multiple Scattering Methodsmentioning
confidence: 99%
“…le Havre) using a formalism, appropriately developed for this case and presented elsewhere. [76,116] Each resonance mode appearing at frequency f (n, l) in these DOS spectra is characterized by the angular momentum l, imposed by the spherical symmetry of the particle, where n denotes the n-th order solution for a given l. All the shell-localized modes reported in this section have n=1. The materials elastic parameters (c l , c t ) and densities are used as adjustable parameters in order to achieve the least deviation between theoretical and experimental eigenfrequencies.…”
Section: The Vibrations Of Individual Colloidsmentioning
confidence: 99%
“…section 3.4.1). [76,95] In the computations, a plane sound wave propagating in air and impinging upon a single PS sphere was considered and after subtracting the scattering amplitude for a rigid sphere of equal size, the sphere eigenmodes appear as resonance peaks in the plot of scattering cross-section versus frequency. Thereby the resonance frequencies f (n, l) can be identified as mode with angular momentum quantum number l of n-th order.…”
Section: Elastic Vibrations In Homogeneous Polymermentioning
“…The calculation for homogeneous spheres can be found in literature [53] as well as the solutions for inhomogeneous core-shell particles. [76] Coming back to our system with N scatterers, the total wave field incident on the n-th scatterer is the sum of the incident plane wave and the wave field scattered from all scatterers n ′ = n.…”
Section: The Multiple Scattering Methodsmentioning
confidence: 99%
“…[40,76,80] For a slab parallel to a distinct crystallographic plane, the reduced vector parallel to this plane, k , is usually a conserved quantity. Therefore, LMS searches in each individual slab propagating Bloch waves for given ω and k , which are the eigenmodes of the elastic field in that slab.…”
Section: The Multiple Scattering Methodsmentioning
confidence: 99%
“…le Havre) using a formalism, appropriately developed for this case and presented elsewhere. [76,116] Each resonance mode appearing at frequency f (n, l) in these DOS spectra is characterized by the angular momentum l, imposed by the spherical symmetry of the particle, where n denotes the n-th order solution for a given l. All the shell-localized modes reported in this section have n=1. The materials elastic parameters (c l , c t ) and densities are used as adjustable parameters in order to achieve the least deviation between theoretical and experimental eigenfrequencies.…”
Section: The Vibrations Of Individual Colloidsmentioning
confidence: 99%
“…section 3.4.1). [76,95] In the computations, a plane sound wave propagating in air and impinging upon a single PS sphere was considered and after subtracting the scattering amplitude for a rigid sphere of equal size, the sphere eigenmodes appear as resonance peaks in the plot of scattering cross-section versus frequency. Thereby the resonance frequencies f (n, l) can be identified as mode with angular momentum quantum number l of n-th order.…”
Section: Elastic Vibrations In Homogeneous Polymermentioning
“…The elastic wave propagation problem through three-dimensional periodic composites formed by arranging spherical scatterers periodically in a homogeneous host matrix with infinite extension has been studied in recent years [1][2][3][4][5]. Compared with the elastic wave propagation through random composites with random distributed spherical scatterers in host material [6][7][8], there are unique band bap effects in the frequency domain for the periodic composites.…”
The work presented in this paper discusses the transmission properties of elastic waves through multilayers of spheres which are periodically arranged in a homogeneous host material. The multilayers of spheres can have different kinds of planar defects. These defects are formed by removing one layer of spheres or by changing the radiuses or the material of scatterers in some layers. First, the reflection and transmission matrices of a single layer of spheres are obtained by the multiple scattering approaches and then the reflection and transmission matrices of multilayers of spheres are derived based on the polymerization method. Numerical examples are presented for 15 layers of spheres with one central planar defect layer or two symmetrically arranged planar defect layers. The influences of these planar defects on the frequency-dependent transmission curves are discussed. It is observed that the band gap can be widened evidently by introducing the planar defect, and the defect states appear in the band gap consequently. So the elaborately arranged planar defects are important in designing specific acoustic filters.
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