2019
DOI: 10.1063/1.5087054
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All-dielectric metasurfaces with trapped modes: Group-theoretical description

Abstract: An all-dielectric metasurface featuring resonant conditions of the trapped mode excitation is considered. It is composed of a lattice of subwavelength particles which are made of a high-refractive-index dielectric material structured in the form of disks. Each particle within the lattice behaves as an individual dielectric resonator supporting a set of electric and magnetic (Mie-type) modes. In order to access a trapped mode (which is the TE 01δ mode of the resonator), a round eccentric penetrating hole is mad… Show more

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Cited by 55 publications
(39 citation statements)
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“…The corresponding quality factors of leaky resonances depend on the degree of the introduced structural asymmetry [20]. The concept of manipulating the transition between the symmetry-protected BICs and leaky resonances was first proposed for plasmonic metasurfaces composed of metallic split-ring resonators [21], and then it was developed for all-dielectric metasurfaces [22][23][24][25][26][27][28][29][30][31]. The recent development in topological photonics has demonstrated a wide class of topologically protected states [32].…”
Section: Introductionmentioning
confidence: 99%
“…The corresponding quality factors of leaky resonances depend on the degree of the introduced structural asymmetry [20]. The concept of manipulating the transition between the symmetry-protected BICs and leaky resonances was first proposed for plasmonic metasurfaces composed of metallic split-ring resonators [21], and then it was developed for all-dielectric metasurfaces [22][23][24][25][26][27][28][29][30][31]. The recent development in topological photonics has demonstrated a wide class of topologically protected states [32].…”
Section: Introductionmentioning
confidence: 99%
“…To explore these selection rules, we employ theoretical-group approach. The group-theoretic approach is a powerful method which is widely used for analyzing the properties of periodic photonic system [30,[49][50][51][52]. In this section, we apply this method to reveal which of the coefficients D piprmn are non-zero in accordance with the mode symmetry imposed by the symmetry of the periodic structure [53,54] and to explain the formation of BIC.…”
Section: Multipolar Approachmentioning
confidence: 99%
“…Such * z.sadrieva@metalab.ifmo.ru † k.frizyuk@metalab.ifmo.ru kind of BIC is called symmetry-protected, and they also allow interpretation in terms of topological charges defined by the number of times the polarization vectors winds around the BICs presented as vortex centers in the polarization field [28]. In contrast to the symmetryprotected BIC, the so-called accidental BICs [1,[28][29][30][31] can be observed out of the Γ-point due to an accidental nulling of the Fourier (coupling) coefficients via fine tuning of parameters of the photonic system. Such a mechanism is also known as Friedrich-Wintgen scenario [32].…”
Section: Introductionmentioning
confidence: 99%
“…These resonances are related to the collective trapped mode excitation. [32][33][34] Therefore, in order to differentiate the features of the cluster-based configuration from those influenced by the particles perturbations, further we consider three particular designs of the metasurface. The first design is realized by displacing the non-perturbed disks toward the unit cell center by a distance s along the cell's diagonals [ Fig.…”
mentioning
confidence: 99%
“…The cluster forming metasurface corresponds to the group C 4v for all chosen designs. 33 This group has the four-fold symmetry axis with respect to rotation around the z axis. For the metasurfaces whose unit cell symmetry belongs to the rotational groups C 4v , there is polarization independence of the structure under normal incidence conditions.…”
mentioning
confidence: 99%