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Volumn 81, Issue 4, 2010, Pages

Implementation of dispersion models in the split-field-finite-difference- time-domain algorithm for the study of metallic periodic structures at oblique incidence

Author keywords

[No Author keywords available]

Indexed keywords

ADDITIONAL EQUATIONS; ANGLE OF INCIDENCE; DISPERSION MODELS; DISPERSIVE MEDIA; ENHANCED TRANSMISSION; FDTD ALGORITHM; FIELD COMPONENTS; FIELD METHODS; FINITE DIFFERENCE TIME-DOMAIN; LORENTZ DISPERSION MODEL; METAL DISPERSIONS; OBLIQUE INCIDENCE;

EID: 77951753084     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.81.046705     Document Type: Article
Times cited : (20)

References (16)
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    • 10.1103/PhysRevE.77.056701
    • A. Belkhir and F. I. Baida, Phys. Rev. E 77, 056701 (2008). 10.1103/PhysRevE.77.056701
    • (2008) Phys. Rev. e , vol.77 , pp. 056701
    • Belkhir, A.1    Baida, F.I.2
  • 4
    • 68949178217 scopus 로고    scopus 로고
    • 10.1364/OL.34.002453
    • F. I. Baida and A. Blekhir, Opt. Lett. 34, 2453 (2009). 10.1364/OL.34.002453
    • (2009) Opt. Lett. , vol.34 , pp. 2453
    • Baida, F.I.1    Blekhir, A.2
  • 6
    • 77951760196 scopus 로고    scopus 로고
    • The Drude model is given by ε (ω) =1- ωp2 ω (ω+iγ ), where ωp is the plasma frequency and γ is associated to the losses.
    • The Drude model is given by ε (ω) = 1 - ω p 2 ω (ω + i γ), where ω p is the plasma frequency and γ is associated to the losses.
  • 9
    • 48749122536 scopus 로고    scopus 로고
    • Proceedings of the International Conference on Nanoscience and Nanotechnology (ICONN 2006), Brisbane, Australia, (IEEE Press, Piscataway, New Jersey
    • R. J. Blaikie, L. Lin, and R. J. Reeves, Proceedings of the International Conference on Nanoscience and Nanotechnology (ICONN 2006), Brisbane, Australia, (IEEE Press, Piscataway, New Jersey, 2006), pp. 458-461.
    • (2006) , pp. 458-461
    • Blaikie, R.J.1    Lin, L.2    Reeves, R.J.3
  • 12
    • 77951722430 scopus 로고    scopus 로고
    • For a perfect conductor, this mode is called TEM mode ( Eφ and Hz are zero). In the case of a real metal, these two components of the guided electromagnetic field can not completely vanish because of the penetration of the field inside the metal.
    • For a perfect conductor, this mode is called TEM mode (Eφ and H z are zero). In the case of a real metal, these two components of the guided electromagnetic field can not completely vanish because of the penetration of the field inside the metal.
  • 13
    • 0036680108 scopus 로고    scopus 로고
    • 10.1016/S0030-4018(02)01690-5
    • F. I. Baida and D. Van Labeke, Opt. Commun. 209, 17 (2002). 10.1016/S0030-4018(02)01690-5
    • (2002) Opt. Commun. , vol.209 , pp. 17
    • Baida, F.I.1    Van Labeke, D.2
  • 15
    • 33847651336 scopus 로고    scopus 로고
    • 10.1038/nnano.2007.53
    • T. Thio, Nat. Nanotechnol. 2, 136 (2007). 10.1038/nnano.2007.53
    • (2007) Nat. Nanotechnol. , vol.2 , pp. 136
    • Thio, T.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.