Fast and accurate electromagnetic field calculation for substrate-supported metasurfaces using the discrete dipole approximation
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Wyant College of Optical Sciences, University of ArizonaIssue Date
2023-10-23Keywords
cylindrical Green's functiondiscrete dipole approximation
finite difference time domain
metasurface
Sommerfeld integral
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Walter de Gruyter GmbHCitation
Liu, Weilin and McLeod, Euan. "Fast and accurate electromagnetic field calculation for substrate-supported metasurfaces using the discrete dipole approximation" Nanophotonics, vol. 12, no. 22, 2023, pp. 4157-4173. https://doi.org/10.1515/nanoph-2023-042Journal
NanophotonicsRights
© 2023 the author(s), published by De Gruyter. This work is licensed under the Creative Commons Attribution 4.0 International License.Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
Metasurface design tends to be tedious and time-consuming based on sweeping geometric parameters. Common numerical simulation techniques are slow for large areas, ultra-fine grids, and/or three-dimensional simulations. Simulation time can be reduced by combining the principle of the discrete dipole approximation (DDA) with analytical solutions for light scattered by a dipole near a flat surface. The DDA has rarely been used in metasurface design, and comprehensive benchmarking comparisons are lacking. Here, we compare the accuracy and speed of three DDA methods - substrate discretization, two-dimensional Cartesian Green's functions, and one-dimensional (1D) cylindrical Green's functions - against the finite difference time domain (FDTD) method. We find that the 1D cylindrical approach performs best. For example, the s-polarized field scattered from a silica-substrate-supported 600 × 180 × 60 nm gold elliptic nanocylinder discretized into 642 dipoles is computed with 0.78 % pattern error and 6.54 % net power error within 294 s, which is 6 times faster than FDTD. Our 1D cylindrical approach takes advantage of parallel processing and also gives transmitted field solutions, which, to the best of our knowledge, is not found in existing tools. We also examine the differences among four polarizability models: Clausius-Mossotti, radiation reaction, lattice dispersion relation, and digitized Green's function, finding that the radiation reaction dipole model performs best in terms of pattern error, while the digitized Green's function has the lowest power error. © 2023 the author(s), published by De Gruyter, Berlin/Boston 2023.Note
Open access journalISSN
2192-8614Version
Final Published Versionae974a485f413a2113503eed53cd6c53
10.1515/nanoph-2023-0423
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Except where otherwise noted, this item's license is described as © 2023 the author(s), published by De Gruyter. This work is licensed under the Creative Commons Attribution 4.0 International License.