1999
DOI: 10.1143/jjap.38.l157
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A Two-Dimensional Photonic Crystal Laser

Abstract: We report on observation of laser action unique to a two-dimensional (2D) photonic lattice. When dye-solution filled in air-holes of a 2D lattice was optically-pumped, laser action without external mirrors is found to occur at a specific wavelength corresponding to a flat band-dispersion in a high-symmetry direction of the 2D lattice plane; a small group-velocity is responsible for the lasing. On further increasing the pump-fluence, another laser action is also found to occur around a peak wavel… Show more

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Cited by 73 publications
(33 citation statements)
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“…The two periodic structures have the same unit cell thickness d, and the FPC length is L Nd = . We assume that the FPC with RBE is constructed from alternating lossless dielectric layers with real refractive indices 1 ) along the z-direction associated to these two coupled waves are described by a four dimensional state vector…”
Section: Giant Gain and The Wigner Time Increasementioning
confidence: 99%
“…The two periodic structures have the same unit cell thickness d, and the FPC length is L Nd = . We assume that the FPC with RBE is constructed from alternating lossless dielectric layers with real refractive indices 1 ) along the z-direction associated to these two coupled waves are described by a four dimensional state vector…”
Section: Giant Gain and The Wigner Time Increasementioning
confidence: 99%
“…PhCs have many attractive characteristics such as photonic bandgap (PBG), localization effect, and refraction effect. By introducing point defect and/or line defect, PhC-based devices can be made [2], such as PhC-based waveguide [3][4][5], nanocavity [6][7][8], low threshold lasers [9][10][11][12], PhC-based filter [13][14][15], PhC fibers [16][17][18][19], optical sensors, and so on.…”
Section: Introductionmentioning
confidence: 99%
“…Compared to conventional Fabry-Perot or DFB edge-emitting lasers, such micro cavity lasers have many interesting characteristics, such as ultra-small size, with the possibility of close-to-diffraction-limited mode volume, ultra-low threshold, and on-chip integration [11][12][13][14][15]. However, because the semiconductor membrane has a thickness of a few hundred nanometers and normally is suspended in air, heat generated through the pumping process, either optical or electrical, may accumulate in the structure, making it difficult to achieve continuous-wave (CW) lasing at room temperature [11][12][13][14]. Even with the achievement of CW lasing, the laser output power saturates when the pump power is only a few times larger than the laser threshold level [16].…”
Section: Introductionmentioning
confidence: 99%