Theoretical models have been developed to investigate the reflection and transmission spectra, and photonic band structure for a midinfrared layer-by-layer metallic photonic crystal. It is found that photonic band gap effects due to global coupling between different unit cells in different layers play a key role in the formation of the lowest stop band gap extending to zero frequency and a high transmission passband adjacent to the stop band gap. Excellent agreement of theoretical results with experimental measurements is achieved.
REFERENCES
1.
2.
3.
M.
Sigalas
, C. T.
Chan
, K. M.
Ho
, and C. M.
Soukoulis
, Phys. Rev. B
52
, 11744
(1995
).4.
D. F.
Sievenpiper
, M. E.
Sickmiller
, and E.
Yablonovitch
, Phys. Rev. Lett.
76
, 2480
(1996
).5.
S.
Fan
, P. R.
Villeneuve
, and J. D.
Joannopoulos
, Phys. Rev. B
54
, 11245
(1996
).6.
E.
Özbay
, B.
Temelkuran
, M.
Sigalas
, G.
Tuttle
, C. M.
Soukoulis
, and K. M.
Ho
, Appl. Phys. Lett.
69
, 3797
(1996
).7.
W.
Zhang
, X. Y.
Lei
, Z. L.
Wang
, D. G.
Zheng
, W. Y.
Tam
, C. T.
Chan
, and P.
Sheng
, Phys. Rev. Lett.
84
, 2853
(2000
).8.
K. M.
Ho
, C. T.
Chan
, C. M.
Soukoulis
, R.
Biswas
, and M.
Sigalas
, Solid State Commun.
89
, 413
(1994
).9.
10.
J. G.
Fleming
, S. Y.
Lin
, I.
El-Kady
, R.
Biswas
, and K. M.
Ho
, Nature (London)
417
, 52
(2002
).11.
T. W.
Ebbesen
, H. J.
Lezec
, H. F.
Ghaemi
, T.
Thio
, and P. A.
Wolff
, Nature (London)
391
, 667
(1998
);H. F.
Ghaemi
, T.
Thio
, D. E.
Grupp
, T. W.
Ebbesen
, and H. J.
Lezec
, Phys. Rev. B
58
, 6779
(1998
).12.
J. A.
Porto
, F. J.
Garcia-Vidal
, and J. B.
Pendry
, Phys. Rev. Lett.
83
, 2845
(1999
).13.
E.
Popov
, M.
Nevieve
, S.
Enoch
, and R.
Reinisch
, Phys. Rev. B
62
, 16100
(2000
).14.
15.
M. G.
Moharam
, E. B.
Grann
, D. A.
Pommet
, and T. K.
Gaylord
, J. Opt. Soc. Am. A
12
, 1068
(1995
);16.
H. Raether, Surface Plasmons on Smooth and Rough Surfaces and on Gratings (Springer, Berlin, 1988).
17.
J. R.
Andrewartha
, J. R.
Fox
, and I. J.
Wilson
, Opt. Acta
26
, 69
(1979
).18.
19.
In Ref. 10, the real-sapce transfer-matrix method was employed to calculate the spectra of the tungsten photonic crystal, and a filling fraction of the tungsten rod was used to fit the experimental parameter of due to limited grid mesh number and the use of a cubic grid cell in the transfer-matrix method for this noncubic lattice. Finer grid mesh was used, but led to poor convergence of the simulated spectra. In the present approach, the exact geometric parameters of the tungsten photonic crystal was adopted without any fitting.
20.
P. M.
Bell
, J. B.
Pendry
, L.
Marin Moreno
, and A. J.
Ward
, Comput. Phys. Commun.
85
, 306
(1995
).
This content is only available via PDF.
© 2003 American Institute of Physics.
2003
American Institute of Physics
You do not currently have access to this content.