2006
DOI: 10.1016/j.photonics.2005.10.002
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From modal control to spontaneous emission and gain in photonic crystal waveguides

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Cited by 14 publications
(8 citation statements)
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“…In practice, if one retains PhC claddings that are unmodified and that consist of circular air holes in a triangular arrangement, there are only small regions of the TM polarization, i.e., E along the hole axis, where we could spot flatband regions. This explains that in spite of a high interest that has been directed toward multimode PhCWGs, including for slow light and related phenomena [23,24,34], no actual strong systematic flattening of the kind reported here has been noticed.…”
Section: (A) and 3(b) Extension Tomentioning
confidence: 48%
See 1 more Smart Citation
“…In practice, if one retains PhC claddings that are unmodified and that consist of circular air holes in a triangular arrangement, there are only small regions of the TM polarization, i.e., E along the hole axis, where we could spot flatband regions. This explains that in spite of a high interest that has been directed toward multimode PhCWGs, including for slow light and related phenomena [23,24,34], no actual strong systematic flattening of the kind reported here has been noticed.…”
Section: (A) and 3(b) Extension Tomentioning
confidence: 48%
“…• Slow light in PhCs has motivated intense investigation in W1 membrane systems [19][20][21], but some studies tackled slow light in larger guides such as W2 and W3 [22,23]. Meanwhile, our group has also pioneered the use of MSBs and a kind of slow light for demultiplexing devices [14,24,25]. How much does our generic approach apply when reducing W (toward low mode numbers m) and thus violating the equidistant-mode assumption?…”
Section: Broad Periodic Waveguidesmentioning
confidence: 99%
“…Dowling et al 12 suggested that the slow down of light near the edge of a one-dimensional photonic bandgap structure could be used to enhance the gain coefficient. The slow propagation of the Bloch mode near the band edge, which may be visualized as multiple back-and-forth scattering of the light beam, thus lengthens the local dwell time in the medium and increases the spatial but not the temporal gain coefficient 13 . Despite obvious applications in optical amplifiers 14,15 and lasers 16 , there is no conclusive experimental demonstration in a waveguide structure.…”
mentioning
confidence: 99%
“…The slow propagation of the Bloch mode near the band edge, which may be visualized as multiple back-and-forth scattering of the light beam, thus lengthens the local dwell time in the medium and increases the spatial but not the temporal gain coefficient. 15 Despite obvious applications in optical amplifiers 16 and lasers, 13 there is no conclusive experimental demonstration in a waveguide structure. For dye-doped 3D artificial opals, enhancement of gain in certain crystallographic directions and its relation to the directional density of optical states was demonstrated 17 and in Ref.…”
mentioning
confidence: 99%
“…The preliminary experiments of Fig.12 exemplify this operation : we started from a wide open section of "W15" PhCW which lases in lateral modes, as we recently reported 33 . We created the gain region by photopuming (using ~40 mW focused from a red laser diode with cylindrical optics).…”
Section: Gain Enhancement and Nonlinear Effectsmentioning
confidence: 64%