2020
DOI: 10.48550/arxiv.2003.10876
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Asymptotic approximations for Bloch waves and topological mode steering in a planar array of Neumann scatterers

Abstract: We study the canonical problem of wave scattering by periodic arrays, either of infinite or finite extent, of Neumann scatterers in the plane; the characteristic lengthscale of the scatterers is considered small relative to the lattice period. We utilise the method of matched asymptotic expansions, together with Fourier series representations, to create an efficient and accurate numerical approach for finding the dispersion curves associated with Floquet-Bloch waves through an infinite array of scatterers. The… Show more

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Cited by 2 publications
(9 citation statements)
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“…A fascinating chiral beaming phenomenon has been observed for classical and electronic valley-Hall systems [12,49]. By exciting a valley-Hall crystal near the periphery of the topological band gap (Fig.…”
Section: B Elastic Edge Waves To Chirality-locked Beam Splittingmentioning
confidence: 97%
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“…A fascinating chiral beaming phenomenon has been observed for classical and electronic valley-Hall systems [12,49]. By exciting a valley-Hall crystal near the periphery of the topological band gap (Fig.…”
Section: B Elastic Edge Waves To Chirality-locked Beam Splittingmentioning
confidence: 97%
“…6(b). The excitation of the π/3 separated ± pseudospin states stems from the gradient direction of the triangular isofrequency contours [12,49].…”
Section: B Elastic Edge Waves To Chirality-locked Beam Splittingmentioning
confidence: 99%
“…We proceed by numerically solving the spectral problem ( 2)-( 4) using the finite element package Comsol Multiphysics [28] to compute the eigenfrequencies Ω k and associated Bloch eigensolutions H k l when k spans the Brillouin zone (BZ) in the reciprocal space. These finite element numerics are complemented by a semi-analytic method based around monopolar and dipolar scattering by small metallic cylinders, the details of which are in [29] and covered briefly in Appendix A. These eigenfrequencies form a discrete spectrum ω j , j = 1, 2 • • • , and noting that Ω ≥ 0 in (2) it is easily seen [4] that these are bounded below with…”
Section: Symmetry Protected Topological States In Hexagonal and Squar...mentioning
confidence: 99%
“…We opt to use an alternative semi-analytical approach that is less computationally expensive than directly using finite element methods and which is relevant to open systems. This method is explained in detail in [29] and is briefly summarised in Appendix A. The usefulness of this semi-analytical scheme will become apparent in Sec.…”
Section: Infinite Array Of Small Circular Perfectly Conducting Cylindersmentioning
confidence: 99%
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