2020
DOI: 10.1109/jphot.2020.2977860
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Resonant Excitation Analysis on Asymmetrical Lateral Leakage of Light in Finite Zero-Contrast Grating Mirror

Abstract: Resonant excitation analysis on asymmetrical lateral leakage of light in the finite zero-contrast grating (ZCG) mirror is demonstrated, and the size effect of the excited source is investigated. The dispersion equation of slab waveguide for the TM mode is proposed to evaluate the resonant condition of the ZCG mirror, and it is shown that the mirror effect of the infinite ZCG is resulted from the overlapping of order-mode resonance pairs. However, two leaky channels are excited in spectra of the finite ZCG mirr… Show more

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Cited by 15 publications
(8 citation statements)
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“…There are different kinds of BICs, classified by their physical origins and constructing methods, including BICs from symmetry or separability, from parameter tuning in resonance systems, and from inverse construction. [ 163 ] BICs and quasi‐BICs have been found in photonic systems such as PC slabs, [ 164–203 ] gratings, [ 204–219 ] metamaterials, [ 220–227 ] coupled waveguide arrays, [ 228–230 ] array of spheres or rods. [ 231–234 ] Here, we will mainly introduce the topology of BICs in PCs.…”
Section: Physics and Designs Of Topological Photonic Crystalsmentioning
confidence: 99%
“…There are different kinds of BICs, classified by their physical origins and constructing methods, including BICs from symmetry or separability, from parameter tuning in resonance systems, and from inverse construction. [ 163 ] BICs and quasi‐BICs have been found in photonic systems such as PC slabs, [ 164–203 ] gratings, [ 204–219 ] metamaterials, [ 220–227 ] coupled waveguide arrays, [ 228–230 ] array of spheres or rods. [ 231–234 ] Here, we will mainly introduce the topology of BICs in PCs.…”
Section: Physics and Designs Of Topological Photonic Crystalsmentioning
confidence: 99%
“…As can be seen in Figure 3 b, there are two leaky mode resonances (LMRs) in the wavelength region of interest as s = 0; the LMRs arise from the coupling between the diffracted orders and the waveguide modes, and the overlapping of the two LMRs will result in broadband reflection with high reflectivity [ 45 ]. However, two additional high-Q Fano resonances occurred as s = 10 nm, where BIC turns into quasi-BIC due to the symmetry-breaking of the structure [ 46 , 47 ]. At normal incidence, the BIC mode can be completely decoupled from the radiation continuum due to its different symmetry, while it can be leaky by breaking the symmetry of the structure [ 48 , 49 ].…”
Section: Basic Principles and Cmt For Absorption Enhancement Of Grmentioning
confidence: 99%
“…However, most of the dielectric nanostructures used to excite QBICs with high Q-factor are complicated, such as asymmetrical nanocrosses [20], asymmetrical nanorings [21], asymmetrical nanobars [22][23][24] and asymmetrical nanorods [25][26][27][28], which are challenging in fabrication due to the requirement of inserting the deep subwavelength slits [20][21][22][23][24] or nanoholes [25][26][27][28] into the photonic structures. Other nanostructures such as the reshaped rectangular bars [29,30] have the increased sharp edges, making them more difficult to be accurately fabricated through conventional lithographic techniques, which reduces the Q-factor and the resonance lifetime of the devices due to the opening of additional leaky channels [31,32]. Moreover, the tilted nanobars [33,34], another type of structures, have difficulties in precisely control of the orientation of the nanobars with the deep subwavelength spaces between the resonators maintained in nanofabrication process.…”
Section: Introductionmentioning
confidence: 99%