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        <identifier>oai:figshare.com:article/31852669</identifier>
        <datestamp>2026-09-30T16:00:23Z</datestamp>
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          <dc:title>Mie-lithography: void-resonance-assisted femtosecond laser printing for deep-ultraviolet to near-infrared nano dispersion devices</dc:title>
          <dc:creator>Wei Gong (112494)</dc:creator>
          <dc:creator>Zhen-Ze Li (15346291)</dc:creator>
          <dc:creator>Chang Yu (237950)</dc:creator>
          <dc:creator>Zhen Wang (72451)</dc:creator>
          <dc:creator>Han-Yue Fan (23621485)</dc:creator>
          <dc:creator>Yi Wang (32470)</dc:creator>
          <dc:creator>Zhi-Hao Chen (688011)</dc:creator>
          <dc:creator>Chun-Qi Jin (22646711)</dc:creator>
          <dc:creator>Yu-Hao Lei (23621488)</dc:creator>
          <dc:creator>Qi-Dai Chen (1768729)</dc:creator>
          <dc:creator>Lei Wang (6656)</dc:creator>
          <dc:creator>Hong-Bo Sun (1459207)</dc:creator>
          <dc:subject>Physics (arXiv)</dc:subject>
          <dc:subject>physics.optics (arXiv)</dc:subject>
          <dc:description>Nanoscale control of optical dispersion is essential for applications ranging from miniaturized spectrometers to color printing, all of which demand broadband spectral tunability. However, the Kramers-Kronig relations impose a fundamental trade-off between dispersion and loss, strictly limiting the design ability of single-material devices across the deep ultraviolet (DUV) to near-infrared (NIR) regimes. Consequently, the fabrication of miniaturized dispersion devices heavily relies on costly nanofabrication or heterogeneous integration. Here we overcome these limitations by shifting the light-matter interaction from solid structure into air-filled voids. We introduce a fabrication strategy termed "Mie-lithography", in which laser printed seed nanocavities excite Mie resonances in air and the resulting localized field enhancement drives the self-assembly of three-dimensionally tunable void-type optical resonators. Because the resonant modes are primarily confined within air voids, this architecture effectively alleviates material-imposed dispersion-loss constraints, allowing on-demand customization of the broadband spectral response. This approach could enable single-step, high-throughput (&gt;= 10^6 pixels/s) printing of dispersion units with a resolution of 63,500 DPI. As a proof of concept, we demonstrate a single-material nano dispersion device for spectral encoding from 200 to 800 nm, with spectral reconstruction using a camera. Our approach can be extended into a platform for ultra-broadband (DUV-NIR) nano devices fabrication and design, opening avenues for high-pixel-density displays and miniaturized spectrometers.</dc:description>
          <dc:date>2026-09-28T00:00:00Z</dc:date>
          <dc:type>Text</dc:type>
          <dc:type>Preprint</dc:type>
          <dc:identifier>10.48550/arXiv.2603.22034</dc:identifier>
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