{"data":{"id":"10.5061/dryad.fxpnvx16v","type":"dois","attributes":{"doi":"10.5061/dryad.fxpnvx16v","prefix":"10.5061","suffix":"dryad.fxpnvx16v","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Choi, Daegwang","nameType":"Personal","affiliation":["Korea University","Gachon University"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-3102-2918","nameIdentifierScheme":"ORCID"}]},{"name":"Lee, Soon-Jae","nameType":"Personal","affiliation":["Korea University"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0009-0007-8012-3543","nameIdentifierScheme":"ORCID"}]},{"name":"Cho, Seung-Woon","nameType":"Personal","affiliation":["Korea University"],"nameIdentifiers":[]},{"name":"Bark, Chan Bin","nameType":"Personal","affiliation":["Hanyang University"],"nameIdentifiers":[]},{"name":"Pak, Seik","nameType":"Personal","affiliation":["Hanyang University"],"nameIdentifiers":[]},{"name":"Shin, Dong-Jin","nameType":"Personal","affiliation":["Korea University"],"nameIdentifiers":[]},{"name":"Park, Moon Jip","nameType":"Personal","affiliation":["Hanyang University"],"nameIdentifiers":[]},{"name":"Gong, Su-Hyun","nameType":"Personal","affiliation":["Korea University"],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-8652-714X","nameIdentifierScheme":"ORCID"}]}],"titles":[{"title":"Data from: Strong interlayer coupling and chiral flat-band cascades in twisted bilayer gratings"}],"publisher":"Dryad","container":{},"publicationYear":2026,"subjects":[{"subject":"FOS: Natural sciences","schemeUri":"https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf","subjectScheme":"fos"},{"subject":"FOS: Nano-technology","schemeUri":"https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf","subjectScheme":"fos"},{"subject":"Nanofabrication","schemeUri":"https://github.com/PLOS/plos-thesaurus","subjectScheme":"PLOS Subject Area Thesaurus"},{"subject":"Nanoscale photonics","schemeUri":"https://github.com/PLOS/plos-thesaurus","subjectScheme":"PLOS Subject Area Thesaurus"},{"subject":"Semiconductors","schemeUri":"https://github.com/PLOS/plos-thesaurus","subjectScheme":"PLOS Subject Area Thesaurus"}],"contributors":[{"name":"Choi, Daegwang","nameType":"Personal","affiliation":["Korea University","Gachon University"],"contributorType":"ContactPerson","nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-3102-2918","nameIdentifierScheme":"ORCID"}]},{"name":"Lee, Soon-Jae","nameType":"Personal","affiliation":["Korea University"],"contributorType":"ContactPerson","nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0009-0007-8012-3543","nameIdentifierScheme":"ORCID"}]},{"name":"Cho, Seung-Woon","nameType":"Personal","affiliation":["Korea University"],"contributorType":"ContactPerson","nameIdentifiers":[]},{"name":"Bark, Chan Bin","nameType":"Personal","affiliation":["Hanyang University"],"contributorType":"ContactPerson","nameIdentifiers":[]},{"name":"Pak, Seik","nameType":"Personal","affiliation":["Hanyang University"],"contributorType":"ContactPerson","nameIdentifiers":[]},{"name":"Shin, Dong-Jin","nameType":"Personal","affiliation":["Korea University"],"contributorType":"ContactPerson","nameIdentifiers":[]},{"name":"Park, Moon Jip","nameType":"Personal","affiliation":["Hanyang University"],"contributorType":"ContactPerson","nameIdentifiers":[]},{"name":"Gong, Su-Hyun","nameType":"Personal","affiliation":["Korea University"],"contributorType":"ContactPerson","nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-8652-714X","nameIdentifierScheme":"ORCID"}]}],"dates":[{"date":"2025-11-20T07:21:29Z","dateType":"Created"},{"date":"2026-07-16T12:46:14Z","dateType":"Submitted"},{"date":"2026-07-28T00:00:00Z","dateType":"Issued"},{"date":"2026-07-28T00:00:00Z","dateType":"Available"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsCitedBy","relatedIdentifier":"10.48550/arxiv.2510.07381","relatedIdentifierType":"DOI"},{"relationType":"IsCitedBy","relatedIdentifier":"10.1126/sciadv.aed8846","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["312021505 bytes"],"formats":[],"version":"4","rightsList":[{"rights":"Creative Commons Zero v1.0 Universal","rightsUri":"https://creativecommons.org/publicdomain/zero/1.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc0-1.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"From atomic crystals to macroscopic material structures, twisted bilayer\n systems have emerged as a promising route to control wave phenomena. In\n few-layer van der Waals (vdW) materials, however, the intrinsically weak\n interlayer coupling typically demands fine control of small twist angles\n to reach magic-angle conditions. Here, we show that one-dimensional\n photonic crystal bilayers can overcome this limitation by accessing a\n regime of strong interlayer coupling—comparable to intralayer coupling.\n This strong coupling enables flat-band formation over a broad angular\n range even at large twist angles. We experimentally realize this regime by\n stacking WS₂ gratings via a two-step lithography method, yielding\n ultra-wide chiral flat-band cascades in magic-angle twisted bilayer\n gratings. Our work not only provides a platform for designing photonic\n applications with a tunable localization but also explores a new regime of\n physics that is unattainable in conventional solid-state-based moiré\n systems.","descriptionType":"Abstract"},{"description":"# Data from: Strong interlayer coupling and chiral flat-band cascades in\n twisted bilayer gratings Dataset DOI:\n [10.5061/dryad.fxpnvx16v](https://doi.org/10.5061/dryad.fxpnvx16v) ##\n Description of the data and file structure This dataset: TBG_data_set.zip\n contains simulated angle-resolved transmittance and circular-dichroism\n spectra, photonic band-structure calculations, near-field electric\n displacement field profiles, and magic-angle/flat-band-width parameter\n sweeps for twisted bilayer photonic gratings, together with supplementary\n substrate-material comparisons and complex refractive index data. All data\n were generated by rigorous coupled-wave analysis (RCWA) and\n finite-difference time-domain (FDTD) simulation and are stored in Excel\n format, with one file per main-text or supplementary figure and one sheet\n per panel or parameter value. ### Files and variables #### File:\n Fig1_Data.xlsx **Description:** This file provides angle-resolved\n transmittance spectra and near-field electric displacement field profiles\n for the twisted bilayer grating. \"Fig1_c_10degree\",\n \"Fig1_c_35degree\", \"Fig1_c_44degree\", and\n \"Fig1_c_64degree\" provide transmittance as a function of\n incidence angle and photon energy at twist angles of 10°, 35°, 44°, and\n 64°. Sheets \"Fig1_d_44degree_xy_bottom\",\n \"Fig1_d_44degree_xy_top\", and \"Fig_1d_44degree_xz\"\n provide the electric displacement field distribution in the xy (bottom and\n top layer) and xz cross-sections at a 44° twist angle. Sheets\n \"Fig1_e_64degree_xy_bottom\", \"Fig1_e_64degree_xy_top\",\n and \"Fig_1e_64degree_xz\" provide the corresponding field\n distributions at a 64° twist angle. **Variables** * Angle (degree) –\n incidence angle * Energy (eV) – photon energy * Transmittance * X, Y, Z\n (nm) – spatial coordinates * Electric displacement field (a.u.) #### File:\n Fig2_Data.xlsx **Description:** This file provides simulated photonic band\n structures of the twisted bilayer grating. Sheets\n \"Fig2_c_Uncoupled\" and \"Fig2_c_Coupled\" provide the\n k_x–energy dispersion of the uncoupled and coupled bands at one twist\n angle. Sheets \"Fig2_d_Uncoupled\" and \"Fig2_d_Coupled\"\n provide the corresponding uncoupled and coupled bands at a second twist\n angle. Sheet \"Fig_2_e\" provides the twist-angle dependence of\n the band separation parameter (s) for the 1st and 2nd bands. Sheet\n \"Fig_2_f\" provides the twist-angle dependence of the flat-band\n width for the 1st and 2nd bands. **Variables** * k_x – in-plane wavevector\n component * Energy (eV) * s – Dimensionless scaling factor for effective\n coupling strength * Twist angle (degree) * Flat band width #### File:\n Fig3_Data.xlsx **Description:** This file provides angle-resolved\n transmittance spectra of the twisted bilayer grating at different twist\n angles. Sheets \"Fig3_d_38degree\" through\n \"Fig3_d_44degree\" provide transmittance maps at twist angles of\n 38°, 40°, 42°, and 44°. Sheets \"Fig3_e_57degree\" through\n \"Fig3_e_66degree\" provide transmittance maps at twist angles of\n 57°, 60°, 63°, and 66°. **Variables** * Angle (degree) – incidence angle *\n Energy (eV) – photon energy * Transmittance #### File: Fig4_Data.xlsx\n **Description:** This file provides circularly polarized transmittance and\n circular dichroism (CD) data. Sheet \"Fig4_a\" provides the CD map\n as a function of incidence angle and energy. Sheets\n \"Fig4_b_left\" and \"Fig4_b_right\" provide the\n corresponding left- and right-handed circularly polarized transmittance\n maps. Sheet \"Fig4_c\" provides the four\n circular-polarization-resolved transmittance spectra (T_LL, T_LR, T_RR,\n T_RL) at a fixed incidence angle. Sheet \"Fig4_d\" provides the\n same four transmittance spectra under a different condition. **Variables**\n * Angle (degree) – incidence angle * Energy (eV) – photon energy * CD –\n Circular dichroism * Transmittance * T_LL, T_LR, T_RR, T_RL –\n circular-polarization-resolved transmittance #### File: Fig4_E_LCP.txt\n **Description:** This file provides the electric field energy density\n distribution in the xy plane for the left circular polarization\n excitation.  **Variables** * X, Y, Z (nm) – spatial coordinates * Electric\n displacement field (a.u.) #### File: Fig4_E_RCP.txt **Description:** This\n file provides the electric field energy density distribution in the xy\n plane for the right circular polarization excitation.  **Variables** * X,\n Y, Z (nm) – spatial coordinates * Electric displacement field (a.u.) ####\n File: FigS3_Data.xlsx **Description:** This file provides calculated\n angle-resolved transmittance spectra at twist angles of 44°, 45°, 46°,\n 47°, 48°, 61°, 62°, 63°, 64°, and 65°, one sheet per angle. **Variables**\n * Angle (degree) – incidence angle * Energy (eV) – photon energy *\n Transmittance #### File: FigS4_Data.xlsx **Description:** This file\n provides the magic angle and flat-band width as a function of grating\n layer thickness. **Variables** * Thickness (nm) * Magic angle (Degree) *\n Flat-band width (Degree) #### File: FigS5_Data.xlsx **Description:** This\n file provides the magic angle and flat-band width as a function of grating\n period. **Variables** * Period (nm) * Magic angle (Degree) * Flat-band\n width (Degree) #### File: FigS6_Data.xlsx **Description:** This file\n provides angle-resolved transmittance spectra at twist angles of 15°, 20°,\n 30°, 45°, 60°, and 70°, one sheet per angle. **Variables** * Angle\n (degree) – incidence angle * Energy (eV) – photon energy * Transmittance\n #### File: FigS7_Data.xlsx **Description:** This file provides uncoupled\n and coupled photonic band structures at twist angles of 40°, 45°, 50°,\n 55°, 60°, and 65°, with separate \"_Uncoupled\" and\n \"_Coupled\" sheets for each angle. **Variables** * Band index *\n k_x in-plane wavevector component * Energy (eV) #### File: FigS8_Data.xlsx\n **Description:** This file provides uncoupled and coupled photonic band\n structures at twist angles of 43°, 44.3°, 47.3°, 49°, 51°, and 53°, with\n separate \"_uncoupled\" and \"_coupled\" sheets for each\n angle. **Variables** * Band index * k_x – in-plane wavevector component *\n Energy (eV) #### File: FigS9_Data.xlsx **Description:** This file provides\n uncoupled and coupled photonic band structures at twist angles of 60.5°,\n 61°, 61.5°, 62°, 63.3°, and 64°, with separate\n \"_Uncoupled/_uncoupled\" and \"_coupled\" sheets for each\n angle. **Variables** * Band index * k_x – in-plane wavevector component *\n Energy (eV) #### File: FigS10_Data.xlsx **Description:** This file\n provides angle-resolved transmittance spectra for two grating\n configurations (\"M1\", \"M2\") at spacer thicknesses of 0\n nm, 40 nm, and 80 nm. **Variables** * Angle (degree) – incidence angle *\n Energy (eV) – photon energy * Transmittance #### File: FigS11_Data.xlsx\n **Description:** This file provides the magic angle and flat-band width as\n a function of interlayer distance. Sheets \"FigS11_a\" and\n \"FigS11_b\" correspond to two different grating configurations.\n **Variables** * Interlayer distance (nm) * Magic angle (Degree) *\n Flat-band width (Degree) #### File: FigS12_Data.xlsx **Description:** This\n file provides circularly polarized transmittance and CD data. Sheet\n \"FigS12_A\" provides the CD map as a function of incidence angle\n and energy. Sheets \"FigS12_B_TRR\", \"FigS12_B_TRL\",\n \"FigS12_B_TLR\", and \"FigS12_B_TLL\" provide the\n corresponding circular-polarization-resolved transmittance maps. Sheets\n \"FigS12_C\" and \"FigS12_D\" provide the four\n circular-polarization-resolved transmittance spectra (T_RR, T_LL, T_LR,\n T_RL) at two fixed incidence angles. **Variables** * Angle (degree) –\n incidence angle * Energy (eV) – photon energy * CD – Circular dichroism *\n Transmittance * T_LL, T_LR, T_RR, T_RL – circular-polarization-resolved\n transmittance #### File: FigS15_Data.xlsx **Description:** This file\n provides angle-resolved transmittance spectra for gratings on three\n different substrate materials: GaP, hBN, and WS2. **Variables** * Angle\n (degree) – incidence angle * Energy (eV) – photon energy * Transmittance\n #### File: FigS16_Data.xlsx **Description:** This file provides the\n complex refractive index of the grating material WS2 as a function of\n wavelength. **Variables** * Wavelength (nm) * Real index * Imaginary index\n #### File: FigS18_Data.xlsx **Description:** This file provides\n angle-resolved transmittance spectra for the y-direction at twist angles\n from 10° to 70° (10°, 20°, 25°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, 65°,\n 70°), one sheet per angle. **Variables** * Angle (degree) – incidence\n angle * Energy (eV) – photon energy * Transmittance ## Code/Software Any\n program that will open a spreadsheet, such as Microsoft Excel is\n recommended.","descriptionType":"TechnicalInfo"}],"geoLocations":[],"fundingReferences":[{"funderName":"National Research Foundation of Korea","awardNumber":"RS-2024-00335222","funderIdentifier":"https://ror.org/013aysd81","funderIdentifierType":"ROR"},{"funderName":"National Research Foundation of Korea","awardNumber":"RS-2025-16070482","funderIdentifier":"https://ror.org/013aysd81","funderIdentifierType":"ROR"},{"funderName":"National Research Foundation of Korea","awardNumber":"RS-2023-00218998","funderIdentifier":"https://ror.org/013aysd81","funderIdentifierType":"ROR"},{"funderName":"National Research Foundation of Korea","awardNumber":"RS-2025-25446099","funderIdentifier":"https://ror.org/013aysd81","funderIdentifierType":"ROR"},{"funderName":"National Research Foundation of Korea","awardNumber":"RS-2025-03392969","funderIdentifier":"https://ror.org/013aysd81","funderIdentifierType":"ROR"},{"funderName":"Samsung Science and Technology Foundation (South Korea)","awardNumber":"SSTF-BA1902-03","funderIdentifier":"https://ror.org/00gjmje40","funderIdentifierType":"ROR"}],"xml":"<?xml version="1.0" encoding="UTF-8"?>
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      <creatorName nameType="Personal">Bark, Chan Bin</creatorName>
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    <creator>
      <creatorName nameType="Personal">Pak, Seik</creatorName>
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    <creator>
      <creatorName nameType="Personal">Shin, Dong-Jin</creatorName>
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    <creator>
      <creatorName nameType="Personal">Park, Moon Jip</creatorName>
      <affiliation affiliationIdentifier="https://ror.org/046865y68" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Hanyang University</affiliation>
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    <creator>
      <creatorName nameType="Personal">Gong, Su-Hyun</creatorName>
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  <titles>
    <title>
      Data from: Strong interlayer coupling and chiral flat-band cascades in
      twisted bilayer gratings
    </title>
  </titles>
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    <subject subjectScheme="fos" schemeURI="https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf">FOS: Natural sciences</subject>
    <subject subjectScheme="fos" schemeURI="https://web-archive.oecd.org/2012-06-15/138575-38235147.pdf">FOS: Nano-technology</subject>
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    <subject subjectScheme="PLOS Subject Area Thesaurus" schemeURI="https://github.com/PLOS/plos-thesaurus">Nanoscale photonics</subject>
    <subject subjectScheme="PLOS Subject Area Thesaurus" schemeURI="https://github.com/PLOS/plos-thesaurus">Semiconductors</subject>
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      <funderName>Samsung Science and Technology Foundation (South Korea)</funderName>
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  <contributors>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Choi, Daegwang</contributorName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0003-3102-2918</nameIdentifier>
      <affiliation affiliationIdentifier="https://ror.org/047dqcg40" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Korea University</affiliation>
      <affiliation affiliationIdentifier="https://ror.org/03ryywt80" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Gachon University</affiliation>
    </contributor>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Lee, Soon-Jae</contributorName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0009-0007-8012-3543</nameIdentifier>
      <affiliation affiliationIdentifier="https://ror.org/047dqcg40" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Korea University</affiliation>
    </contributor>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Cho, Seung-Woon</contributorName>
      <affiliation affiliationIdentifier="https://ror.org/047dqcg40" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Korea University</affiliation>
    </contributor>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Bark, Chan Bin</contributorName>
      <affiliation affiliationIdentifier="https://ror.org/046865y68" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Hanyang University</affiliation>
    </contributor>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Pak, Seik</contributorName>
      <affiliation affiliationIdentifier="https://ror.org/046865y68" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Hanyang University</affiliation>
    </contributor>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Shin, Dong-Jin</contributorName>
      <affiliation affiliationIdentifier="https://ror.org/047dqcg40" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Korea University</affiliation>
    </contributor>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Park, Moon Jip</contributorName>
      <affiliation affiliationIdentifier="https://ror.org/046865y68" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Hanyang University</affiliation>
    </contributor>
    <contributor contributorType="ContactPerson">
      <contributorName nameType="Personal">Gong, Su-Hyun</contributorName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0002-8652-714X</nameIdentifier>
      <affiliation affiliationIdentifier="https://ror.org/047dqcg40" affiliationIdentifierScheme="ROR" schemeURI="https://ror.org">Korea University</affiliation>
    </contributor>
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  <dates>
    <date dateType="Created">2025-11-20T07:21:29Z</date>
    <date dateType="Submitted">2026-07-16T12:46:14Z</date>
    <date dateType="Issued">2026-07-28T00:00:00Z</date>
    <date dateType="Available">2026-07-28T00:00:00Z</date>
  </dates>
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    <relatedIdentifier relationType="IsCitedBy" relatedIdentifierType="DOI">https://doi.org/10.1126/sciadv.aed8846</relatedIdentifier>
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  <descriptions>
    <description descriptionType="Abstract">
      From atomic crystals to macroscopic material structures, twisted bilayer
      systems have emerged as a promising route to control wave phenomena. In
      few-layer van der Waals (vdW) materials, however, the intrinsically weak
      interlayer coupling typically demands fine control of small twist angles
      to reach magic-angle conditions. Here, we show that one-dimensional
      photonic crystal bilayers can overcome this limitation by accessing a
      regime of strong interlayer coupling—comparable to intralayer coupling.
      This strong coupling enables flat-band formation over a broad angular
      range even at large twist angles. We experimentally realize this regime by
      stacking WS₂ gratings via a two-step lithography method, yielding
      ultra-wide chiral flat-band cascades in magic-angle twisted bilayer
      gratings. Our work not only provides a platform for designing photonic
      applications with a tunable localization but also explores a new regime of
      physics that is unattainable in conventional solid-state-based moiré
      systems.
    </description>
    <description descriptionType="TechnicalInfo">
      # Data from: Strong interlayer coupling and chiral flat-band cascades in
      twisted bilayer gratings Dataset DOI:
      [10.5061/dryad.fxpnvx16v](https://doi.org/10.5061/dryad.fxpnvx16v) ##
      Description of the data and file structure This dataset: TBG_data_set.zip
      contains simulated angle-resolved transmittance and circular-dichroism
      spectra, photonic band-structure calculations, near-field electric
      displacement field profiles, and magic-angle/flat-band-width parameter
      sweeps for twisted bilayer photonic gratings, together with supplementary
      substrate-material comparisons and complex refractive index data. All data
      were generated by rigorous coupled-wave analysis (RCWA) and
      finite-difference time-domain (FDTD) simulation and are stored in Excel
      format, with one file per main-text or supplementary figure and one sheet
      per panel or parameter value. ### Files and variables #### File:
      Fig1_Data.xlsx **Description:** This file provides angle-resolved
      transmittance spectra and near-field electric displacement field profiles
      for the twisted bilayer grating. "Fig1_c_10degree",
      "Fig1_c_35degree", "Fig1_c_44degree", and
      "Fig1_c_64degree" provide transmittance as a function of
      incidence angle and photon energy at twist angles of 10°, 35°, 44°, and
      64°. Sheets "Fig1_d_44degree_xy_bottom",
      "Fig1_d_44degree_xy_top", and "Fig_1d_44degree_xz"
      provide the electric displacement field distribution in the xy (bottom and
      top layer) and xz cross-sections at a 44° twist angle. Sheets
      "Fig1_e_64degree_xy_bottom", "Fig1_e_64degree_xy_top",
      and "Fig_1e_64degree_xz" provide the corresponding field
      distributions at a 64° twist angle. **Variables** * Angle (degree) –
      incidence angle * Energy (eV) – photon energy * Transmittance * X, Y, Z
      (nm) – spatial coordinates * Electric displacement field (a.u.) #### File:
      Fig2_Data.xlsx **Description:** This file provides simulated photonic band
      structures of the twisted bilayer grating. Sheets
      "Fig2_c_Uncoupled" and "Fig2_c_Coupled" provide the
      k_x–energy dispersion of the uncoupled and coupled bands at one twist
      angle. Sheets "Fig2_d_Uncoupled" and "Fig2_d_Coupled"
      provide the corresponding uncoupled and coupled bands at a second twist
      angle. Sheet "Fig_2_e" provides the twist-angle dependence of
      the band separation parameter (s) for the 1st and 2nd bands. Sheet
      "Fig_2_f" provides the twist-angle dependence of the flat-band
      width for the 1st and 2nd bands. **Variables** * k_x – in-plane wavevector
      component * Energy (eV) * s – Dimensionless scaling factor for effective
      coupling strength * Twist angle (degree) * Flat band width #### File:
      Fig3_Data.xlsx **Description:** This file provides angle-resolved
      transmittance spectra of the twisted bilayer grating at different twist
      angles. Sheets "Fig3_d_38degree" through
      "Fig3_d_44degree" provide transmittance maps at twist angles of
      38°, 40°, 42°, and 44°. Sheets "Fig3_e_57degree" through
      "Fig3_e_66degree" provide transmittance maps at twist angles of
      57°, 60°, 63°, and 66°. **Variables** * Angle (degree) – incidence angle *
      Energy (eV) – photon energy * Transmittance #### File: Fig4_Data.xlsx
      **Description:** This file provides circularly polarized transmittance and
      circular dichroism (CD) data. Sheet "Fig4_a" provides the CD map
      as a function of incidence angle and energy. Sheets
      "Fig4_b_left" and "Fig4_b_right" provide the
      corresponding left- and right-handed circularly polarized transmittance
      maps. Sheet "Fig4_c" provides the four
      circular-polarization-resolved transmittance spectra (T_LL, T_LR, T_RR,
      T_RL) at a fixed incidence angle. Sheet "Fig4_d" provides the
      same four transmittance spectra under a different condition. **Variables**
      * Angle (degree) – incidence angle * Energy (eV) – photon energy * CD –
      Circular dichroism * Transmittance * T_LL, T_LR, T_RR, T_RL –
      circular-polarization-resolved transmittance #### File: Fig4_E_LCP.txt
      **Description:** This file provides the electric field energy density
      distribution in the xy plane for the left circular polarization
      excitation.  **Variables** * X, Y, Z (nm) – spatial coordinates * Electric
      displacement field (a.u.) #### File: Fig4_E_RCP.txt **Description:** This
      file provides the electric field energy density distribution in the xy
      plane for the right circular polarization excitation.  **Variables** * X,
      Y, Z (nm) – spatial coordinates * Electric displacement field (a.u.) ####
      File: FigS3_Data.xlsx **Description:** This file provides calculated
      angle-resolved transmittance spectra at twist angles of 44°, 45°, 46°,
      47°, 48°, 61°, 62°, 63°, 64°, and 65°, one sheet per angle. **Variables**
      * Angle (degree) – incidence angle * Energy (eV) – photon energy *
      Transmittance #### File: FigS4_Data.xlsx **Description:** This file
      provides the magic angle and flat-band width as a function of grating
      layer thickness. **Variables** * Thickness (nm) * Magic angle (Degree) *
      Flat-band width (Degree) #### File: FigS5_Data.xlsx **Description:** This
      file provides the magic angle and flat-band width as a function of grating
      period. **Variables** * Period (nm) * Magic angle (Degree) * Flat-band
      width (Degree) #### File: FigS6_Data.xlsx **Description:** This file
      provides angle-resolved transmittance spectra at twist angles of 15°, 20°,
      30°, 45°, 60°, and 70°, one sheet per angle. **Variables** * Angle
      (degree) – incidence angle * Energy (eV) – photon energy * Transmittance
      #### File: FigS7_Data.xlsx **Description:** This file provides uncoupled
      and coupled photonic band structures at twist angles of 40°, 45°, 50°,
      55°, 60°, and 65°, with separate "_Uncoupled" and
      "_Coupled" sheets for each angle. **Variables** * Band index *
      k_x in-plane wavevector component * Energy (eV) #### File: FigS8_Data.xlsx
      **Description:** This file provides uncoupled and coupled photonic band
      structures at twist angles of 43°, 44.3°, 47.3°, 49°, 51°, and 53°, with
      separate "_uncoupled" and "_coupled" sheets for each
      angle. **Variables** * Band index * k_x – in-plane wavevector component *
      Energy (eV) #### File: FigS9_Data.xlsx **Description:** This file provides
      uncoupled and coupled photonic band structures at twist angles of 60.5°,
      61°, 61.5°, 62°, 63.3°, and 64°, with separate
      "_Uncoupled/_uncoupled" and "_coupled" sheets for each
      angle. **Variables** * Band index * k_x – in-plane wavevector component *
      Energy (eV) #### File: FigS10_Data.xlsx **Description:** This file
      provides angle-resolved transmittance spectra for two grating
      configurations ("M1", "M2") at spacer thicknesses of 0
      nm, 40 nm, and 80 nm. **Variables** * Angle (degree) – incidence angle *
      Energy (eV) – photon energy * Transmittance #### File: FigS11_Data.xlsx
      **Description:** This file provides the magic angle and flat-band width as
      a function of interlayer distance. Sheets "FigS11_a" and
      "FigS11_b" correspond to two different grating configurations.
      **Variables** * Interlayer distance (nm) * Magic angle (Degree) *
      Flat-band width (Degree) #### File: FigS12_Data.xlsx **Description:** This
      file provides circularly polarized transmittance and CD data. Sheet
      "FigS12_A" provides the CD map as a function of incidence angle
      and energy. Sheets "FigS12_B_TRR", "FigS12_B_TRL",
      "FigS12_B_TLR", and "FigS12_B_TLL" provide the
      corresponding circular-polarization-resolved transmittance maps. Sheets
      "FigS12_C" and "FigS12_D" provide the four
      circular-polarization-resolved transmittance spectra (T_RR, T_LL, T_LR,
      T_RL) at two fixed incidence angles. **Variables** * Angle (degree) –
      incidence angle * Energy (eV) – photon energy * CD – Circular dichroism *
      Transmittance * T_LL, T_LR, T_RR, T_RL – circular-polarization-resolved
      transmittance #### File: FigS15_Data.xlsx **Description:** This file
      provides angle-resolved transmittance spectra for gratings on three
      different substrate materials: GaP, hBN, and WS2. **Variables** * Angle
      (degree) – incidence angle * Energy (eV) – photon energy * Transmittance
      #### File: FigS16_Data.xlsx **Description:** This file provides the
      complex refractive index of the grating material WS2 as a function of
      wavelength. **Variables** * Wavelength (nm) * Real index * Imaginary index
      #### File: FigS18_Data.xlsx **Description:** This file provides
      angle-resolved transmittance spectra for the y-direction at twist angles
      from 10° to 70° (10°, 20°, 25°, 30°, 35°, 40°, 45°, 50°, 55°, 60°, 65°,
      70°), one sheet per angle. **Variables** * Angle (degree) – incidence
      angle * Energy (eV) – photon energy * Transmittance ## Code/Software Any
      program that will open a spreadsheet, such as Microsoft Excel is
      recommended.
    </description>
  </descriptions>
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