Coherent Control of Wave Beams Via Unidirectional Evanescent Modes Excitation
Conventional coherent absorption occurs only when two incident beams exhibit mirror symmetry with respect to the absorbing surface, i.e., the two beams have the same incident angles, phases, and amplitudes. This study proposes a more general metasurface paradigm for coherent perfect absorption with...
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Veröffentlicht in: | Advanced functional materials 2023-11, Vol.33 (48), p.n/a |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Conventional coherent absorption occurs only when two incident beams exhibit mirror symmetry with respect to the absorbing surface, i.e., the two beams have the same incident angles, phases, and amplitudes. This study proposes a more general metasurface paradigm for coherent perfect absorption with impinging waves from arbitrary asymmetric directions. By exploiting excitation of unidirectional evanescent waves, the output can be fixed at one reflection direction for any amplitude and phase of the control wave. It shows theoretically and confirm experimentally that the relative amplitude of the reflected wave can be tuned continuously from zero to unity by changing the phase difference between the two beams, i.e., switching from coherent perfect absorption to full reflection. It hopes that this study will open up promising possibilities for wave manipulation via evanescent waves engineering with applications in optical switches, optical computing, one‐side sensing, photovoltaics, and radar cross‐section control.
Conventional coherent perfect absorption occurs only when two incident beams exhibit mirror symmetry with respect to the absorbing surface. Here, a gradient coherent metasurface paradigm by exploiting excitation of unidirectional evanescent waves is proposed, achieving coherent perfect absorption and single‐direction reflection for illuminations from the same side at two or more arbitrary angles in different phase scenarios, respectively. |
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ISSN: | 1616-301X 1616-3028 |
DOI: | 10.1002/adfm.202304300 |