2008 10th Anniversary International Conference on Transparent Optical Networks 2008
DOI: 10.1109/icton.2008.4598620
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Effect of Gain Saturation in InP-Photonic Band Gap Active Waveguides

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Cited by 4 publications
(7 citation statements)
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“…The other physical and geometrical parameters are: core thickness d c = 110.5 nm, refractive index n AlGaAs = 3.285 and thickness d cl = 0.220 µm of the cladding, ridge width w = 2 μm and the two values of the ridge height h 1 = 0.1 µm and h 2 = 1.0 µm. The interaction of the injected current with the active 4-QW structure, has been accounted by using the following rate equations [10,17]:…”
Section: Brief Theorymentioning
confidence: 99%
See 1 more Smart Citation
“…The other physical and geometrical parameters are: core thickness d c = 110.5 nm, refractive index n AlGaAs = 3.285 and thickness d cl = 0.220 µm of the cladding, ridge width w = 2 μm and the two values of the ridge height h 1 = 0.1 µm and h 2 = 1.0 µm. The interaction of the injected current with the active 4-QW structure, has been accounted by using the following rate equations [10,17]:…”
Section: Brief Theorymentioning
confidence: 99%
“…In more recent years, the PhCs have offered novel possibilities for controlling [9][10][11][12] and filtering [13-16] the propagating light signals in integrated optical devices even in presence of active materials [17,18].…”
Section: Introductionmentioning
confidence: 99%
“…In particular, the behaviour of the examined structure is deeply affected by the interaction of the injected current with the active materials acting along the whole structure. This effect is accounted by introducing in the computer code the following rate equations in the stationary analysis [18,19]:…”
Section: Design Of the Active Wdm Filtermentioning
confidence: 99%
“…Moreover, in presence of dielectric discontinuity this algorithm solves both the forward (+z) and the backward (−z) propagations along the longitudinal z direction of the waveguiding structure. The MoL-BBPM procedure, applied iteratively by evaluating the whole electromagnetic field in the structure, stops when the change of the electromagnetic field, at the generic i-th iteration, in the output section is less than a given tolerance ε [26]:…”
Section: Brief Theorymentioning
confidence: 99%
“…Moreover, the PBG devices are even more interesting when exploiting different material properties, e.g., in the case of liquid crystal infiltration or nonlinear materials [23,24], which allow the realization of efficient tunable filters and frequency converters. Moreover, they exhibit a more efficient interaction between the light and the active materials, thanks to their capability of reducing the group velocity at certain wavelengths [25,26].…”
Section: Introductionmentioning
confidence: 99%