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One of the important advantages of optical metasurfaces over conventional diffractive optical elements is their capability to efficiently deflect light by large angles. However, metasurfaces are conventionally designed using approaches that are optimal for small deflection angles and their performance for designing high numerical aperture devices is not well quantified. Here we introduce and apply a technique for the estimation of the efficiency of high numerical aperture metasurfaces. The technique is based on a particular coherent averaging of diffraction coefficients of periodic blazed gratings and can be used to compare the performance of different metasurface designs in implementing high numerical aperture devices. Unlike optimization-based methods that rely on full-wave simulations and are only practicable in designing small metasurfaces, the gradient averaging technique allows for the design of arbitrarily large metasurfaces. Using this technique, we identify an unconventional metasurface design and experimentally demonstrate a metalens with a numerical aperture of 0.78 and a measured focusing efficiency of 77%. The grating averaging is a versatile technique applicable to many types of gradient metasurfaces, thus enabling highly efficient metasurface components and systems.
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http://dx.doi.org/10.1038/s41598-020-64198-8 | DOI Listing |
Sci Rep
September 2025
Center for X-ray and Nano Science CXNS, Deutsches Elektronen-Synchrotron DESY, Notkestraße 85, 22607, Hamburg, Germany.
In-situ imaging of chemical reactions can provide valuable insight into nanoparticle growth and structural evolution. Hard X-ray imaging is an excellent tool for this purpose, as it combines high spatial resolution with high penetration depth, allowing for realistic reaction environments. While far-field ptychography is a well-established method at synchrotron radiation sources, its near-field analog has received less attention.
View Article and Find Full Text PDFLight Sci Appl
August 2025
School of Mechanical Science and Engineering, Huazhong University of Science and Technology, Wuhan, Hubei, China.
Coherent diffractive imaging (CDI), with its lensless geometry and theoretically perfect transfer function, is considered as one of the most promising paradigms to achieve the Abbe resolution limit. However, recent advances on pushing the resolution limit in high-numerical-aperture (NA) CDIs has thus far been challenging. Here, we report a nearly 0.
View Article and Find Full Text PDFSci Adv
August 2025
Physics Department and Institute of Nanotechnology and Advanced Materials, Bar-Ilan University, Ramat Gan 52900, Israel.
The resolution of a measurement system is fundamentally constrained by the wavelength of the used wave packet and the numerical aperture of the optical system. Overcoming these limits requires advanced interferometric techniques exploiting quantum correlations. While quantum interferometry can surpass the Heisenberg limit, it has been confined to the optical domain.
View Article and Find Full Text PDFHigh-performance polarization-multiplexed metalenses (PMMs) hold remarkable transformative potential in optical platforms. However, balancing the numerical aperture (NA), focusing efficiency, and spectral bandwidth remains a significant challenge in the existing PMMs, thus restricting their extensive applications. To circumvent these challenges, we theoretically demonstrate two unique orthogonal (linear and circular) PMMs based on all 4H-silicon carbide (4H-SiC) with superior NA, sound focusing efficiency, and broad wavelength range.
View Article and Find Full Text PDFWe demonstrate a submillimeter-length single-helix chiral grating embedded in a high-numerical-aperture single-mode fiber (HNA-SMF) for efficient generation of third-order orbital angular momentum (OAM), specifically the OAM mode. This design facilitates enhanced coupling of higher azimuthal modes due to significant perturbations arising from both the geometric effect of the thin-core offset under high-NA conditions and the elasto-optic effect induced by intense helical stress with a small twist pitch. As a result, we achieve an unprecedented device length of 0.
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