2001
DOI: 10.1049/el:20010195
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Singlemode transmission within photonic bandgapofwidth-varied single-line-defect photonic crystal waveguideson SOI substrates

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Cited by 118 publications
(57 citation statements)
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“…The W1 PCW attracts interest as it supports a single spatially even mode on most of the photonic band gap. Such a system has been thoroughly investigated on membrane structures [1][2][3][4][5][6][7], where lossless modes exist below the light cone. A membrane-based structure is a very interesting object of study, but injecting light in the structure still remains challenging [8]; furthermore, for any in-plane optical function, the design will probably break the PC translational symmetry, then light is not transmitted anymore on lossless modes.…”
Section: Introductionmentioning
confidence: 99%
“…The W1 PCW attracts interest as it supports a single spatially even mode on most of the photonic band gap. Such a system has been thoroughly investigated on membrane structures [1][2][3][4][5][6][7], where lossless modes exist below the light cone. A membrane-based structure is a very interesting object of study, but injecting light in the structure still remains challenging [8]; furthermore, for any in-plane optical function, the design will probably break the PC translational symmetry, then light is not transmitted anymore on lossless modes.…”
Section: Introductionmentioning
confidence: 99%
“…If two pulses centered at the carrier frequencies and , propagate in opposite directions with wave vectors and , and group velocities and , respectively, the space representation of the field is (37) The interference pattern of the spectral components of this field (for example, considering the component at from the forward-propagating pulse and the component at of the backward-propagating pulse) is weighted by a complex coupling coefficient which depends on the material properties, the orientation of the medium, and the polarization of the waves [27], [31]. Therefore, we may write the grating as (38) where is the total optical power. Equation (38), describing the refractive index, may be used to express the nonlinear polarization as in standard coupled-mode theory [27]; the formalism presented in Section IV then dictates the polarization-driven evolution of the fields.…”
Section: B Two-wave and Four-wave Coupling Via Index Gratingsmentioning
confidence: 99%
“…Therefore, we may write the grating as (38) where is the total optical power. Equation (38), describing the refractive index, may be used to express the nonlinear polarization as in standard coupled-mode theory [27]; the formalism presented in Section IV then dictates the polarization-driven evolution of the fields. The particular example of photorefractive holography, which introduces the further complication of two time coordinates, separated by the hold-time of the grating is discussed elsewhere [6].…”
Section: B Two-wave and Four-wave Coupling Via Index Gratingsmentioning
confidence: 99%
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“…Several examples are illustrated in figure 2.12. In figure 2.12(a), the waveguide is designed by shifting the lattice so the distance between the adjacent rows of columns is reduced γ times the distance of the original waveguide [Not01]. In figure 2.12(b), the radius of the adjacent rows of columns that form the waveguide is changed [Adi00].…”
Section: Fundamentals Of Photonic Crystalsmentioning
confidence: 99%