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Modified Theory of Physical Optics Approach To Diffraction by an Interface Between Pemc and Absorbing Half-Planes

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Date

2021

Journal Title

Journal ISSN

Volume Title

Publisher

Lgep-supelec

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Green Open Access

No

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Abstract

The scattering of electromagnetic plane waves by an interface, located between perfect electromagnetic conductor and absorbing half-planes, is investigated. The perfect electromagnetic conductor half-plane is divided into perfect electric conductor and perfect magnetic conductor half-screens. The same decomposition is done for the absorbing surface. Then four different geometries are defined according to this approach. The scattered fields by the four sub-problems are obtained with the aid of the modified theory of physical optics. The resultant scattering integrals are combined in a single expression by using key formulas, defined for the perfect electromagnetic conductor and absorbing surfaces. The diffracted and geometric optics fields are obtained by the asymptotic evaluation of the scattering integral for large values of the wave-number. The behaviors of the derived field expressions are analyzed numerically.

Description

Keywords

Diffraction Theory, High-Frequency Techniques, Modified Theory Of Physical Optics, Perfect Absorber, Perfect Electromagnetic Conductor, Electricity and magnetism, QC501-766, Physics, QC1-999, Diffraction theory, High-frequency techniques, Modified theory of physical optics, Perfect absorber, Perfect electromagnetic conductor.

Fields of Science

0103 physical sciences, 0202 electrical engineering, electronic engineering, information engineering, 02 engineering and technology, 01 natural sciences

Citation

Umul, Yusuf Z...at all (2021). "Modified Theory of Physical Optics Approach to Diffraction by an Interface between PEMC and Absorbing Half-Planes", Advanced Electromagnetics, Vol. 10, No. 2, pp. 78-84.

WoS Q

Q4

Scopus Q

Q3
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OpenCitations Citation Count
2

Source

Advanced Electromagnetics

Volume

10

Issue

2

Start Page

78

End Page

84
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Scopus : 2

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2

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1

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3

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0.2635166

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