2013
DOI: 10.1364/ol.38.000163
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Controlling the spectral width in compound waveguide grating structures

Abstract: Spectral responses in compound waveguide grating structures composed of two ridges with identical widths in each period are presented. For the proposed structures, we show that the spectral width of the guided-mode resonance (GMR) can be tailored in an independent way without modifying the spectral lineshapes and sideband levels. The method described in this Letter offers a very simple and efficient way to control spectral responses in GMR structures.

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Cited by 53 publications
(27 citation statements)
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“…As d/p decreases from 1 to 0, the responsivity peaks tend to move along a line of the same order FP resonance. According to effective medium theory, [34][35][36] a subwavelength grating can be replaced by a homogeneous, isotropic layer with an appropriate effective index. The effective indices of a 1D subwavelength grating are given by…”
Section: Resultsmentioning
confidence: 99%
“…As d/p decreases from 1 to 0, the responsivity peaks tend to move along a line of the same order FP resonance. According to effective medium theory, [34][35][36] a subwavelength grating can be replaced by a homogeneous, isotropic layer with an appropriate effective index. The effective indices of a 1D subwavelength grating are given by…”
Section: Resultsmentioning
confidence: 99%
“…It is generally accepted that blazed, compound, and complex gratings can be harnessed for the design of spectral and spatial distribution of transmitted, reflected, and guided light modes with improved desired properties such as enhancement or improved coherence of emitted radiation [150]. These kinds of grating can be used for beam shaping [151,152], spectroscopy [153], and spectral filtering [154]. Coherent SP radiation, generated by the passage of relativistic short-bunched electrons across the surface of a metallic grating, has been observed in the wavelength region from 0.5 to 4.0 mm [155].…”
Section: Smith-purcell Sourcesmentioning
confidence: 99%
“…Assume that the total width of the two grating grooves in each period is kept constant, that is, fb+fc=0.4. According to the rigorous coupled-wave theory [22], the grating Fourier harmonics εn control the amplitude of evanescent diffraction fields and are responsible for the mutual interaction of the evanescent diffraction fields, which have the following forms [23]:ε0=1fbfcnSi2+fb+fcnAir2,εn=nSi2nAir2sinnπ1fcsinnπfbnπ, where nSi and nAir represent the refractive indexes of silicon and air, respectively. n is equal to ±1,±2,±normalN…”
Section: Design For Two-part-period and Three-part-period Gratingsmentioning
confidence: 99%