2008
DOI: 10.1063/1.2907488
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Lasing from dye-doped photonic crystals with graded layers in dichromate gelatin emulsions

Abstract: We report on optically pumped lasing from dye-doped, graded-spacing layer structures of dichromate gelatin emulsions fabricated using two-beam holographic interference. The graded layers exhibited deep and wide photonic band gaps. Multimode lasing with both a low threshold and a high quality factor was observed at the band edge of the photonic band gap. We modeled the emissions from the dye-doped graded layer system using a finite difference time domain technique and achieved good agreement with experimental r… Show more

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Cited by 27 publications
(25 citation statements)
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“…Figure 5C demonstrates the linewidth of the random lasing mode at 568.83 nm, which is 0.048 nm as described as full-width at half-maximum (FWHM; Δλ). The corresponding quality factor (defined as λ peak /Δλ) of 11,851 is improved by 1667% (625%) with respect to that of the Ag nanowires [39] (nanoparticles [40])-based random lasers and is comparable to other lasing systems [41,42]. The stability of the random laser is concluded in Figure S6 (Supporting Information) by demonstrating the threshold variations of the 1-year-stored Ag NF-based random lasers at different times, displaying a stable threshold behavior with little fluctuations around 0.24 MW cm −2 , which is the same as that of the random laser shown in Figure 5B.…”
Section: Resultsmentioning
confidence: 79%
“…Figure 5C demonstrates the linewidth of the random lasing mode at 568.83 nm, which is 0.048 nm as described as full-width at half-maximum (FWHM; Δλ). The corresponding quality factor (defined as λ peak /Δλ) of 11,851 is improved by 1667% (625%) with respect to that of the Ag nanowires [39] (nanoparticles [40])-based random lasers and is comparable to other lasing systems [41,42]. The stability of the random laser is concluded in Figure S6 (Supporting Information) by demonstrating the threshold variations of the 1-year-stored Ag NF-based random lasers at different times, displaying a stable threshold behavior with little fluctuations around 0.24 MW cm −2 , which is the same as that of the random laser shown in Figure 5B.…”
Section: Resultsmentioning
confidence: 79%
“…Holography has shown good potential in fabricating PCs [10,11,13,34,35]. Recent research shows that the 1D PC and quasicrystals PC, with gradual distribution of the refractive index materials made by holography using DCG, can also achieve band edge lasing [36,37]. Using DCG, the present authors fabricated a 3D lattice structure which achieved wide band gaps [38], and sometimes achieved complete band gaps [39,40].…”
Section: Band Edge Lasermentioning
confidence: 94%
“…In our experiments, the measured structure was pumped by a ns pulsed Nd:YAG laser with a pulse duration of 8 ns and a ps pulsed Nd:YAG laser with a pulse duration of 30 ps. The pulse laser with a repetition rate of 10 Hz is the most common commercial equipment in wide use, for example, in the work of [36] and [37]. Therefore, such lasers running at 532 nm and repetition rates of 10 Hz were used.…”
Section: Experimental Methods and The Samplesmentioning
confidence: 99%
“…One kind of the PC-based lasers can occur without external feedback, which the standing wave solution of the Bloch waves at the band edge can be regarded as the feedback source. Such kind of laser has been investigated extensively [127][128][129][130][131][132][133][134]. However, all previous works focus on the PC with high refractive index material.…”
Section: Microlaser Realized By Low Refractive Index Materialsmentioning
confidence: 99%
“…In recent years, there has been a great deal of interests in studying different types of lasers made by the PC [124][125][126][127][128][129][130][131][132][133][134]. One kind of the PC-based lasers can occur without external feedback, which the standing wave solution of the Bloch waves at the band edge can be regarded as the feedback source.…”
Section: Microlaser Realized By Low Refractive Index Materialsmentioning
confidence: 99%