2008
DOI: 10.2528/pierl08022201
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Scalar Equations for Scattering by Rotationally Symmetric Radially Inhomogeneous Anisotropic Sphere

Abstract: Abstract-A set of scalar differential equations for treating scattering by rotationally symmetric radially inhomogeneous anisotropic sphere is presented. These equations may easily be treated by applying the integral equation method that has been developed. Besides a possible different expansion in a Neumann series is also discussed.

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Cited by 9 publications
(6 citation statements)
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“…The investigations of interactions between electromagnetic (E.M.) waves and the anisotropic dielectric targets and their applications have become increasingly important in recent years, particularly in the areas of remote-sensing and detection [1][2][3][4][5][6]. The E.M. wave's propagation in the uniaxial anisotropic medium is researched [7] by using the transmission matrix, however this wave propagation in a general anisotropic dielectric material could not be studied.…”
Section: Introductionmentioning
confidence: 99%
“…The investigations of interactions between electromagnetic (E.M.) waves and the anisotropic dielectric targets and their applications have become increasingly important in recent years, particularly in the areas of remote-sensing and detection [1][2][3][4][5][6]. The E.M. wave's propagation in the uniaxial anisotropic medium is researched [7] by using the transmission matrix, however this wave propagation in a general anisotropic dielectric material could not be studied.…”
Section: Introductionmentioning
confidence: 99%
“…The scattering problems have been surveyed by many authors [32][33][34][35][36][37][38][39][40][41][42]. Here, we consider a thin wire scatterer and obtain the current induced on it.…”
Section: Examplementioning
confidence: 99%
“…The transformation function h (t) is hence chosen to be f (t) for R 1 < t < R 2 in order to make the fields matched at the connected boundary. The scattering characteristics of this reshaped cloaking can be further examined by analytically calculating the field distribution [18][19][20][21][22][23][24][25][26][27][28]. Following the same steps of [7] and [9], we decompose the fields into TE and TM modes by introducing vector potentialsĀ TM andĀ TE , respectively [9]:…”
Section: D Perfect Cloak Created With Segments Of Cylindrical and Spmentioning
confidence: 99%