2007
DOI: 10.1364/ao.46.007942
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Design of a wavelength independent grating in the resonance domain

Abstract: We propose using blazed gratings in the resonance domain with period larger than the wavelength for anti-reflection and polarization selection. The inherent problem in this region is wavelength dispersion, which is solved by analyzing the total reflectivity and electric field distribution. The positional relationship between the area of strong electric field, and the side and tip of the grating is crucial to the wavelength dispersion of total reflectivity.

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Cited by 11 publications
(12 citation statements)
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“…The main differences between the results for Λ/λ of 9.1 and 22.7 are as follows: (1) different peak positions of the angular distribution, (2) broadening of angular distribution by the single-slit effect for Λ/λ of 9.1, and (3) reduction in the total reflectivity for Λ/λ of 22.7 [6].…”
Section: Discussionmentioning
confidence: 85%
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“…The main differences between the results for Λ/λ of 9.1 and 22.7 are as follows: (1) different peak positions of the angular distribution, (2) broadening of angular distribution by the single-slit effect for Λ/λ of 9.1, and (3) reduction in the total reflectivity for Λ/λ of 22.7 [6].…”
Section: Discussionmentioning
confidence: 85%
“…The NS-FDTD program was run under MathCAD T M 2004 (MathSoft Engineering and Education, Inc., Cambridge, USA) [23][24][25]. The detailed calculation conditions are described in a previous paper [6]. The calculated grating is shown in Fig.…”
Section: Simulation Methodsmentioning
confidence: 99%
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“…The sample used was an infinite triangular grating fabricated on a 2-mm-thick transparent acrylic plate. After UV curing the grating was removed from a metallic mold [24]. The grating had periods of 3 and 5 µm and v/w = 1 and d/w = 0.48.…”
Section: Experimental Diffraction Intensity For An Infinite Gratingmentioning
confidence: 99%