2020
DOI: 10.1109/lpt.2020.2972749
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Broadband High-Efficiency Gratings Operating at the 2nd Order Designed by Simplified Modal Method

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Cited by 13 publications
(4 citation statements)
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“…In order to maximize the diffraction efficiency of the (−1, 0) diffraction order under TE and TM polarizations, the grating parameters (h 1 , h 2 , h 3 , d, f ) are selected for optimization. Simultaneously, the optimal solution is filtered by the simulated annealing algorithm [33], which can greatly improve the efficiency of the optimization. The optimized structural parameters are h 1 = 606 nm, h 2 = 492 nm, h 3 = 502 nm, d = 1526 nm and f = 0.607.…”
Section: Investigations and Resultsmentioning
confidence: 99%
“…In order to maximize the diffraction efficiency of the (−1, 0) diffraction order under TE and TM polarizations, the grating parameters (h 1 , h 2 , h 3 , d, f ) are selected for optimization. Simultaneously, the optimal solution is filtered by the simulated annealing algorithm [33], which can greatly improve the efficiency of the optimization. The optimized structural parameters are h 1 = 606 nm, h 2 = 492 nm, h 3 = 502 nm, d = 1526 nm and f = 0.607.…”
Section: Investigations and Resultsmentioning
confidence: 99%
“…The grating structure was made up of rectangular Multilayer-dielectric-film gratings are simpler to create than polarization-independent broadband gratings, and they have a higher efficiency than single-layer dielectric film gratings. Z. Yin, J. Yu, et al [60] created a broadband high-efficiency three-layer all-dielectric rectangular-slot transmission grating with −2 order Bragg incidence in 2020. The three layer structures are composed of Al 2 O 3 , TiO 2 , and SiO 2 .…”
Section: Multilayer Dielectric Film Transmission Gratingmentioning
confidence: 99%
“…At the same time, the above structural parameters are optimized by simulated annealing (SA) algorithm to quickly find the highest diffraction efficiency at two polarizations. SA algorithm is a fast and effective optimization technique to find global solutions by skipping a certain probability of local minima [42]. The optimized structural parameters are h 1 =102 nm, h 2 =495 nm, h 3 =558 nm and f = 0.52.…”
Section: Parameter Optimization and E-field Distributionmentioning
confidence: 99%