2022
DOI: 10.1002/adma.202203956
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Ultrathin Suspended Chiral Metasurfaces for Enantiodiscrimination

Abstract: Chiral metasurfaces can exhibit a strong circular dichroism, but it is limited by the complicated fabrication procedure and alignment errors. Here, a new type of self‐aligned suspended chiral bilayer metasurface with only one‐step electron beam lithography exposure is demonstrated. A significant optical chirality of 221° µm−1 can be realized using suspended metasurfaces with a thickness of 100 nm. Furthermore, this study experimentally demonstrates that such a structure is capable of label‐free discrimination … Show more

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Cited by 25 publications
(23 citation statements)
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“…It can be clearly seen from Figure S6 that the core–shell UCNPs are distributed uniformly over the film, and there is no obvious CD signal in the visible-NIR regime, which further confirms that the CD response is mainly attributed to the suspended bilayer chiral metasurface. As known, electromagnetic fields with intense optical chirality can be formed in the near field of plasmonic chiral nanostructures. ,, Subsequently, we have used the finite-difference time-domain (FDTD) method to simulate the localized optical chirality (indicating the cross-coupling intensity between the magnetic and electric fields) distribution at the XY ( Z = 0 and 26 nm) plane with LCP and RCP incident light (at the CD peak of 830 nm). Figures b and S7 exhibit that the optical chirality is mainly localized in the close vicinity of the Au nanostructures, hence presenting a remarkable asymmetric distribution for LCP and RCP incident light at the wavelength of 830 nm.…”
Section: Resultsmentioning
confidence: 99%
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“…It can be clearly seen from Figure S6 that the core–shell UCNPs are distributed uniformly over the film, and there is no obvious CD signal in the visible-NIR regime, which further confirms that the CD response is mainly attributed to the suspended bilayer chiral metasurface. As known, electromagnetic fields with intense optical chirality can be formed in the near field of plasmonic chiral nanostructures. ,, Subsequently, we have used the finite-difference time-domain (FDTD) method to simulate the localized optical chirality (indicating the cross-coupling intensity between the magnetic and electric fields) distribution at the XY ( Z = 0 and 26 nm) plane with LCP and RCP incident light (at the CD peak of 830 nm). Figures b and S7 exhibit that the optical chirality is mainly localized in the close vicinity of the Au nanostructures, hence presenting a remarkable asymmetric distribution for LCP and RCP incident light at the wavelength of 830 nm.…”
Section: Resultsmentioning
confidence: 99%
“…Additionally, asymmetric transmission, namely, the difference in optical response between backward (i.e., from bottom to top) and forward (i.e., from top to bottom) incidence, is an extraordinary chiroptical effect in the planar chiral structures. Thus, we have also experimentally measured the asymmetric transmission of the chiral metasurface via backward and forward incidence. In Figure S5c and d, the CD curves from backward and forward incidence show a difference in peak position and intensity, which is ascribed to the asymmetric transmission of LCP and RCP through the bilayer chiral metasurface . As a control experiment, the core–shell UCNPs were also spin-coated on a blank Si 3 N 4 film to characterize the CD properties.…”
Section: Resultsmentioning
confidence: 99%
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