Manipulation of Backscattering From a Dielectric Cylinder of Triangular Cross-Section Using the Interplay of Go-Like Ray Effects and Resonances

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Date

2015

Journal Title

Journal ISSN

Volume Title

Publisher

IEEE-Inst Electrical Electronics Engineers Inc

Open Access Color

BRONZE

Green Open Access

Yes

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62

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96

Publicly Funded

No
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Abstract

A triangular dielectric cylinder (dielectric prism) of the size, in cross-section, comparable to or moderately larger than the wavelength is a scatterer, which blends together two different types of electromagnetic behavior: geometrical optics (GO) and resonance. As shown in this paper, the first is responsible, for instance, for enhanced reflection from an isosceles 90 degrees prism, if illuminated from the base. The second is responsible for the peaks in the total scattering and absorption cross-sections (ACSs) at the natural-mode frequencies. The numerical analysis is performed by solving the well-conditioned Muller-type boundary integral equation (IE) discretized using an algorithm with controlled accuracy.

Description

Nosich, Alexander/0000-0002-3446-8168; Altintas, Ayhan/0000-0002-3501-4010

Keywords

Dielectric Prism, Muller Integral Equation (IE), Natural Resonances, Radar Cross-Section (RCS), Scattering, natural resonances, Dielectric prisms, 535, Triangular cross-sections, Resonance, Enhanced reflections, Dielectric cylinder, Scattering, radar cross-section (RCS), Cylinders (shapes), Boundary integral equations, Integral equations, Electromagnetic behavior, Muller integral equation (IE), scattering, Radar cross-section (RCS), Prisms, Radar cross section, 541, Geometrical optics, Dielectric prism, Dielectric devices, Total scattering, Natural resonance

Fields of Science

02 engineering and technology, 0202 electrical engineering, electronic engineering, information engineering

Citation

WoS Q

Q1

Scopus Q

Q1
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OpenCitations Citation Count
21

Source

IEEE Transactions on Antennas and Propagation

Volume

63

Issue

5

Start Page

2162

End Page

2169
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21

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21

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3

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2

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