Abstract
We explore electromagnetic (EM) wave incidence upon gratings of reconfigurable metamaterial cylinders, which collectively act as a metagrating, to identify their potential as reconfigurable subwavelength surfaces. The metacylinders are created by a closely spaced, microstructured array of thin plates that, in the limit of small inter-plate spacing, are described by a semi-analytical continuum model. We build upon metacylinder analysis in water waves, translating this to EM for TE polarization (longitudinal magnetic field) for which the metacylinders exhibit anisotropic scattering; this is exploited for the multiple scattering of light by an infinite metagrating of uniform cylinder radius and angle, for which we retrieve the far-field reflection and transmission spectra for plane-wave incidence. These spectra reveal unusual effects including perfect reflection and a negative Goos–Hänchen shift in the transmitted field, as well as perfect symmetry in the far-field scattering coefficients. The metagrating also hosts Rayleigh–Bloch surface waves, whose dispersion is contingent on the uniform cylinder angle, shifting under rotation towards the light-line as the cylinder angle approaches the horizontal. For both plane-wave scattering and the calculation of the array-guided modes, the cylinder angle is the principal variable in determining the wave interaction, and the metagrating is tunable simply through rotation of the constituent metacylinders.home
Original language | English |
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Article number | 20220454 |
Number of pages | 22 |
Journal | Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences |
Volume | 478 |
Issue number | 2268 |
Early online date | 14 Dec 2022 |
DOIs | |
Publication status | Published - 21 Dec 2022 |
Bibliographical note
Funding Information:H.J.P. is grateful for EPSRC (UK) funding provided through the Centre for Doctoral Training 'Fluid Dynamics Across Scales' Programme (grant no. EP/L016230/1. R.V).
Funding Information:
H.J.P. is grateful for EPSRC (UK) funding provided through the Centre for Doctoral Training ‘Fluid Dynamics Across Scales’ Programme (grant no. EP/L016230/1. R.V). R.V.C. received funding from the European Union’s Horizon 2020 FET Open programme (grant agreement no. 863179 Boheme). H.J.P. and R.V.C. thank QinetiQ Ltd for discussions and the provision of an EPSRC Industrial CASE award, which funded the primary author. R.P. is grateful for the support from the EPSRC (grant no. EP/V04740X/1). S.G. is grateful for the funding provided by the EPSRC (grant no. EP/T002654/1). Acknowledgements
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