2007
DOI: 10.1364/josab.24.003040
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Polarization-independent omnidirectional defect modes in Bragg gaps of one-dimensional photonic crystals

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Cited by 13 publications
(2 citation statements)
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“…[13][14][15] Unusual transmission features can be realized when defects are made of a left-handed material, for example, enabling multiple-wavelength omnidirectional filters. 16 The defect-mode originated transmittance can be interpreted in terms of an equivalent Fabry-Pérot resonator with either planar mirrors placed at virtual interfaces of a PC ͑in the both cases of multiple narrow defects and a single wide defect͒, or volumetric mirrors representing pieces of a regular PC, which delimit a wide defect working as a resonator. 13 In a lossless case, defect modes lead to the total-transmission peaks.…”
Section: Introductionmentioning
confidence: 99%
“…[13][14][15] Unusual transmission features can be realized when defects are made of a left-handed material, for example, enabling multiple-wavelength omnidirectional filters. 16 The defect-mode originated transmittance can be interpreted in terms of an equivalent Fabry-Pérot resonator with either planar mirrors placed at virtual interfaces of a PC ͑in the both cases of multiple narrow defects and a single wide defect͒, or volumetric mirrors representing pieces of a regular PC, which delimit a wide defect working as a resonator. 13 In a lossless case, defect modes lead to the total-transmission peaks.…”
Section: Introductionmentioning
confidence: 99%
“…The concept of photonic crystal (PC) structure was first introduced by Yablonovitch [1] and Sanjeev John [2] in their early work of 1987. A PC is an artificial material with a periodic modulation of its dielectric constant and having ranges of forbidden frequencies called photonic bandgaps (PBGs), analogous to electric bandgaps in semiconductors [3]. PCs have attracted a great deal of attention as a new optical material in recent years [1,[4][5][6][7][8].…”
Section: Introductionmentioning
confidence: 99%