1951
DOI: 10.1103/revmodphys.23.287
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Multiple Scattering of Waves

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Cited by 1,145 publications
(469 citation statements)
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References 66 publications
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“…The saturation effect of the 1D density of states due to disorder is well known, 35 and can be calculated for instance by using the effective-medium model and the coherent-potential approximation ͑CPA͒. 36 However this calculation does not take into account the dissipation such as intrinsic out-of-plane losses. We develop here a simple 1D transfer quasiperiodic matrix model involving the effective indices of the modes of the 2D system to estimate quantitatively the amount of disorder as well as of dissipation.…”
Section: One-dimensional Modeling Of the Disorder And Of The Dissmentioning
confidence: 99%
“…The saturation effect of the 1D density of states due to disorder is well known, 35 and can be calculated for instance by using the effective-medium model and the coherent-potential approximation ͑CPA͒. 36 However this calculation does not take into account the dissipation such as intrinsic out-of-plane losses. We develop here a simple 1D transfer quasiperiodic matrix model involving the effective indices of the modes of the 2D system to estimate quantitatively the amount of disorder as well as of dissipation.…”
Section: One-dimensional Modeling Of the Disorder And Of The Dissmentioning
confidence: 99%
“…. When positional and orientational degrees of freedom are statistically independent, the result of averaging over positional disorder is known to be a sum of two terms describing the coherent and the incoherent scattering [10,29,35]. So, we have…”
Section: Scattering Mean Free Pathmentioning
confidence: 99%
“…At the same time, a wave traveling through an assemblage of isotropic point scatterers can be described by an effective wavenumber whose phase velocity and rate of attenuation depend on (i) the wavenumber of the background medium, (ii) the scatterer density and (iii) the average strength of the scatterers. We note that isotropic point scattering is not essential for the description of a heterogeneous medium by an effective wavenumber (Lax 1951;Waterman & Truell 1961).…”
Section: At T E N Uat I O N O F T H E a M B I E N T S E I S M I C F Imentioning
confidence: 99%
“…At the same time, a wave traveling through an assemblage of isotropic point scatterers can be described by an effective wavenumber whose phase velocity and rate of attenuation depend on (i) the wavenumber of the background medium, (ii) the scatterer density and (iii) the average strength of the scatterers. We note that isotropic point scattering is not essential for the description of a heterogeneous medium by an effective wavenumber (Lax 1951;Waterman & Truell 1961).The total wavefield at a location r can be described as the sum of the background wavefield 0 and the wavefield due to the scatterers s , that is,Since the medium in which the scatterers are embedded is assumed lossless and homogeneous, propagation in this background medium is described by a real wavenumber k 0 . Similarly, the velocity of the background medium is denoted by c 0 and its wavelength by λ 0 .…”
mentioning
confidence: 99%