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Volumn 79, Issue 15, 2009, Pages

Broadband negative refraction with a crossed wire mesh

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EID: 66349132442     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.153109     Document Type: Article
Times cited : (43)

References (20)
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    • 10.1103/PhysRevE.70.046616
    • C. R. Simovski and P. A. Belov, Phys. Rev. E 70, 046616 (2004). 10.1103/PhysRevE.70.046616
    • (2004) Phys. Rev. e , vol.70 , pp. 046616
    • Simovski, C.R.1    Belov, P.A.2
  • 18
    • 66349130272 scopus 로고    scopus 로고
    • For frequencies larger than the plasma frequency, it may be possible that a plane wave propagating in air excites two propagating modes in the metamaterial and thus originates two refracted beams. However in the long wavelength regime considered here, ββp, only a single propagating mode can be excited, and thus there is a single refracted beam.
    • For frequencies larger than the plasma frequency, it may be possible that a plane wave propagating in air excites two propagating modes in the metamaterial and thus originates two refracted beams. However in the long wavelength regime considered here, ββp, only a single propagating mode can be excited, and thus there is a single refracted beam.
  • 20
    • 66349117538 scopus 로고    scopus 로고
    • In nonlocal media the Poynting vector can be explicitly calculated as S= S (0) + S (1), where S (0) = 1 2 Re { E× H} and the "high- frequency" component S (1) is such that Sl (1) =- ω ε0 4 Re { Eε̄ ̄ kl E }, (l=1,2,3) (Refs.). It is demonstrated in Ref. (pp. 65-67) that the Poynting vector is given by the product of the energy density and the group velocity.
    • In nonlocal media the Poynting vector can be explicitly calculated as S= S (0) + S (1), where S (0) = 1 2 Re { E× H} and the "high- frequency" component S (1) is such that Sl (1) =- ω ε0 4 Re { Eε̄ ̄ kl E }, (l=1,2,3) (Refs.). It is demonstrated in Ref. (pp. 65-67) that the Poynting vector is given by the product of the energy density and the group velocity.


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