DocumentCode
3133660
Title
Ideal boundary conditions and the generalized soft-and-hard surface
Author
Lindell, I.V.
Author_Institution
Electromagn. Lab., Helsinki Univ. of Technol., Espoo, Finland
fYear
2000
fDate
2000
Firstpage
333
Lastpage
336
Abstract
The electromagnetic ideal boundary is defined as a surface on which the complex Poynting vector has no normal component. Examples of such boundaries are the classical perfect electric and magnetic boundaries as well as the soft-and-hard surface. In the present study the most general isotropic and anisotropic ideal boundaries are introduced and the basic properties of plane-wave reflection from a planar boundary are studied in terms of incident plane waves. At the isotropic ideal boundary, an incident wave is reflected in two directions. A special self-dual ideal planar boundary has the interesting property as being a perfect back-reflector for a plane wave incident from any direction. An anisotropic ideal boundary can be labeled as a generalized soft-and-hard surface and it can be used to transform the polarization of an incident field to another one
Keywords
electromagnetic field theory; electromagnetic wave polarisation; electromagnetic wave reflection; anisotropic ideal boundaries; complex Poynting vector; electromagnetic ideal boundary; generalised soft/hard surface; generalized soft-and-hard surface; ideal boundary conditions; incident plane waves; isotropic ideal boundaries; perfect back-reflector; planar boundary; plane-wave reflection; polarization transformation; self-dual ideal planar boundary; Anisotropic magnetoresistance; Boundary conditions; Conductors; Corrugated surfaces; Electromagnetic fields; Electromagnetic wave polarization; Laboratories; Magnetic anisotropy; Perpendicular magnetic anisotropy; Reflection;
fLanguage
English
Publisher
ieee
Conference_Titel
Microwave Conference, 2000 Asia-Pacific
Conference_Location
Sydney, NSW
Print_ISBN
0-7803-6435-X
Type
conf
DOI
10.1109/APMC.2000.925806
Filename
925806
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