Controlling electromagnetic surface waves with conformal transformation optics

The application of transformation optics to the development of intriguing electromagnetic devices can produce weakly anisotropic or isotropic media with the assistance of quasi-conformal and/or conformal mapping, as opposed to the strongly anisotropic media produced by general mappings; however, it...

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Bibliographic Details
Published inCommunications physics Vol. 6; no. 1; pp. 201 - 8
Main Authors Zhao, Xiaoyu, Deng, Hong, Gao, Xiaoke, Ma, Xikui, Dong, Tianyu
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 05.08.2023
Nature Publishing Group
Nature Portfolio
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Summary:The application of transformation optics to the development of intriguing electromagnetic devices can produce weakly anisotropic or isotropic media with the assistance of quasi-conformal and/or conformal mapping, as opposed to the strongly anisotropic media produced by general mappings; however, it is typically limited to two-dimensional applications. By addressing the conformal mapping between two manifolds embedded in three-dimensional space, we demonstrate that electromagnetic surface waves can be controlled without introducing singularity and anisotropy into the device parameters. Using fruitful surface conformal parameterization methods, a near-perfect conformal mapping between smooth manifolds with arbitrary boundaries can be obtained. Illustrations of concealing and illusions, including surface Luneburg and Eaton lenses and black holes for surface waves, are provided. Our work brings the manipulation of surface waves at microwave and optical wavelengths one step closer. Transformation optics has shown a powerful way in controlling the light flow. This study provides the conformal mapping between two manifolds embedded in three-dimensional space, enabling the control of surface electromagnetic waves on arbitrary two-dimensional manifold and potentially extends to other fields such as acoustics, mechanics, and thermodynamics.
ISSN:2399-3650
2399-3650
DOI:10.1038/s42005-023-01322-w