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All-angle zero reflection at metamaterial surfaces
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10.1063/1.3012375
/content/aip/journal/apl/93/17/10.1063/1.3012375
http://aip.metastore.ingenta.com/content/aip/journal/apl/93/17/10.1063/1.3012375
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Equifrequency surface analysis of reflection on surfaces of metamaterials with (a) an elliptic and [(b)–(d)] a hyperbolic dispersion. Surfaces (dashed-dotted lines) lie in the horizontal plane. For metamaterials with the hyperbolic dispersion, surfaces are cut along the principal axis (b), perpendicularly to the asymptote (dashed lines) of the hyperbolic dispersion (d) and obliquely to both the principal axis and asymptote (c). Black (gray) thick arrows denote the incident (reflected) wave vector. Thin arrows indicate the direction of the group velocity. Dotted lines illustrate the conservation of the in-plane wave vectors. Note that metamaterials occupy the half-space below the horizontal line and waves are incident from the metamaterial side.

Image of FIG. 2.
FIG. 2.

FDTD simulations of the magnetic field distributions for a -polarized Gaussian beam launched from a periodic metal-dielectric layered structure upon an interface between the structure (gray area) and a dielectric medium (white area) with a dielectric constant of 2.5.

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/content/aip/journal/apl/93/17/10.1063/1.3012375
2008-10-31
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: All-angle zero reflection at metamaterial surfaces
http://aip.metastore.ingenta.com/content/aip/journal/apl/93/17/10.1063/1.3012375
10.1063/1.3012375
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