{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,9,29]],"date-time":"2026-09-29T20:22:50Z","timestamp":1790713370415,"version":"4.1.0"},"reference-count":40,"publisher":"Wiley","issue":"10","license":[{"start":{"date-parts":[[2025,12,22]],"date-time":"2025-12-22T00:00:00Z","timestamp":1766361600000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/creativecommons.org\/licenses\/by\/4.0\/"},{"start":{"date-parts":[[2025,12,22]],"date-time":"2025-12-22T00:00:00Z","timestamp":1766361600000},"content-version":"tdm","delay-in-days":0,"URL":"http:\/\/doi.wiley.com\/10.1002\/tdm_license_1.1"}],"funder":[{"DOI":"10.13039\/501100000781","name":"European Research Council","doi-asserted-by":"publisher","award":["101086683"],"award-info":[{"award-number":["101086683"]}],"id":[{"id":"10.13039\/501100000781","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100004359","name":"Vetenskapsr\u00e5det","doi-asserted-by":"publisher","award":["2020\u201000287"],"award-info":[{"award-number":["2020\u201000287"]}],"id":[{"id":"10.13039\/501100004359","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100004063","name":"Knut och Alice Wallenbergs Stiftelse","doi-asserted-by":"publisher","award":["2019.0163"],"award-info":[{"award-number":["2019.0163"]}],"id":[{"id":"10.13039\/501100004063","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["advanced.onlinelibrary.wiley.com"],"crossmark-restriction":true},"short-container-title":["Advanced Materials"],"published-print":{"date-parts":[[2026,2]]},"abstract":"<jats:title>ABSTRACT<\/jats:title>\n                  <jats:p>\n                    Organic metasurfaces based on conducting polymers are emerging as new opportunities for active nano\u2010optic devices, but their tunable plasmonic resonances are limited to infrared wavelengths (\u2265960\u00a0nm) and mainly with low quality\u2010factors (\n                    <jats:italic>Q<\/jats:italic>\n                    &lt; 2). Here we propose the concept of a \u201cconducting polymer gate\u201d to endow organic metasurfaces with switchable high\u2010\n                    <jats:italic>Q<\/jats:italic>\n                    nonlocal resonances within the visible\/NIR\u2010I regime (640\u2013950\u00a0nm). Poly(3,4\u2010ethylenedioxythiophene) (PEDOT) is integrated into organic dielectric nanocylinder lattices and serves as a gate that controls optical leakage from the nanocylinders to the substrate. The quasi\u2010metallic PEDOT blocks such leakage channel and induces light confinement within the dielectric nanocylinders despite their low refractive index (\n                    <jats:italic>n<\/jats:italic>\n                    <jats:sub>die<\/jats:sub>\n                    &lt; 1.7). This facilitates the generation of Mie collective lattice resonances (CLRs) at the air superstrate with\n                    <jats:italic>Q<\/jats:italic>\n                    \u2010factor reaching 25, which is \u223c16 times higher than previously reported organic metasurfaces near this spectral regime. Converting the PEDOT into its dielectric state opens the leakage channel and eliminates the CLRs, which can be reversibly switched by redox reactions. The concept of conducting polymer\u2010gated optical confinement in low\u2010index nanostructures provides new routes for intelligent nano\u2010optics including dynamic nonlocal metasurfaces.\n                  <\/jats:p>","DOI":"10.1002\/adma.202520674","type":"journal-article","created":{"date-parts":[[2025,12,22]],"date-time":"2025-12-22T08:15:09Z","timestamp":1766391309000},"update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":3,"title":["Dynamic Optical Lattices Through Conducting Polymer\u2010Gated Confinement"],"prefix":"10.1002","volume":"38","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-9311-6197","authenticated-orcid":false,"given":"Dongqing","family":"Lin","sequence":"first","affiliation":[{"name":"Laboratory of Organic Electronics, Department of Science and Technology (ITN) Link\u00f6ping University  Norrk\u00f6ping Sweden"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0009-0000-5748-2854","authenticated-orcid":false,"given":"Yulong","family":"Duan","sequence":"additional","affiliation":[{"name":"Laboratory of Organic Electronics, Department of Science and Technology (ITN) Link\u00f6ping University  Norrk\u00f6ping Sweden"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0001-7816-8602","authenticated-orcid":false,"given":"Suraya","family":"Kazi","sequence":"additional","affiliation":[{"name":"Laboratory of Organic Electronics, Department of Science and Technology (ITN) Link\u00f6ping University  Norrk\u00f6ping Sweden"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-3002-3639","authenticated-orcid":false,"given":"Magnus P.","family":"Jonsson","sequence":"additional","affiliation":[{"name":"Laboratory of Organic Electronics, Department of Science and Technology (ITN) Link\u00f6ping University  Norrk\u00f6ping Sweden"}],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"311","published-online":{"date-parts":[[2025,12,22]]},"reference":[{"key":"e_1_2_12_2_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41563\u2010020\u20100778\u20105"},{"key":"e_1_2_12_3_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41586\u2010022\u201004400\u20101"},{"key":"e_1_2_12_4_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41928\u2010024\u201001293\u2010y"},{"key":"e_1_2_12_5_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41560\u2010022\u201000997\u20109"},{"key":"e_1_2_12_6_1","doi-asserted-by":"publisher","DOI":"10.1021\/acs.nanolett.4c05856"},{"key":"e_1_2_12_7_1","doi-asserted-by":"publisher","DOI":"10.1126\/sciadv.abd9450"},{"key":"e_1_2_12_8_1","doi-asserted-by":"publisher","DOI":"10.1021\/ja054915v"},{"key":"e_1_2_12_9_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41565\u2010019\u20100583\u2010y"},{"key":"e_1_2_12_10_1","doi-asserted-by":"publisher","DOI":"10.1126\/science.abj3433"},{"key":"e_1_2_12_11_1","doi-asserted-by":"publisher","DOI":"10.1039\/D4TC03038A"},{"key":"e_1_2_12_12_1","doi-asserted-by":"publisher","DOI":"10.1002\/adma.202107172"},{"key":"e_1_2_12_13_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41467\u2010022\u201034494\u20100"},{"key":"e_1_2_12_14_1","doi-asserted-by":"publisher","DOI":"10.1039\/D4TC00950A"},{"key":"e_1_2_12_15_1","doi-asserted-by":"publisher","DOI":"10.1002\/lpor.202100633"},{"key":"e_1_2_12_16_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41467\u2010025\u201059764\u20105"},{"key":"e_1_2_12_17_1","doi-asserted-by":"publisher","DOI":"10.1021\/acs.nanolett.3c00772"},{"key":"e_1_2_12_18_1","doi-asserted-by":"publisher","DOI":"10.1126\/sciadv.adh2353"},{"key":"e_1_2_12_19_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41566\u2010021\u201000903\u2010x"},{"key":"e_1_2_12_20_1","doi-asserted-by":"publisher","DOI":"10.1126\/sciadv.abe4553"},{"key":"e_1_2_12_21_1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.90.075404"},{"key":"e_1_2_12_22_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41563\u2010024\u201002042\u20104"},{"key":"e_1_2_12_23_1","doi-asserted-by":"publisher","DOI":"10.1515\/nanoph\u20102023\u20100562"},{"key":"e_1_2_12_24_1","doi-asserted-by":"publisher","DOI":"10.1002\/adfm.202501916"},{"key":"e_1_2_12_25_1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevLett.120.253902"},{"key":"e_1_2_12_26_1","doi-asserted-by":"publisher","DOI":"10.34133\/research.0027"},{"key":"e_1_2_12_27_1","doi-asserted-by":"publisher","DOI":"10.1038\/ncomms1691"},{"key":"e_1_2_12_28_1","doi-asserted-by":"publisher","DOI":"10.1063\/1.5094122"},{"key":"e_1_2_12_29_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsnano.0c00185"},{"key":"e_1_2_12_30_1","doi-asserted-by":"publisher","DOI":"10.1063\/5.0008026"},{"key":"e_1_2_12_31_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.mee.2008.12.057"},{"key":"e_1_2_12_32_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsnano.9b03191"},{"key":"e_1_2_12_33_1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.95.155423"},{"key":"e_1_2_12_34_1","doi-asserted-by":"publisher","DOI":"10.1098\/rspa.2015.0870"},{"key":"e_1_2_12_35_1","doi-asserted-by":"publisher","DOI":"10.1364\/OL.445411"},{"key":"e_1_2_12_36_1","doi-asserted-by":"publisher","DOI":"10.1038\/nphoton.2017.142"},{"key":"e_1_2_12_37_1","doi-asserted-by":"publisher","DOI":"10.1103\/RevModPhys.82.2257"},{"key":"e_1_2_12_38_1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.95.165119"},{"key":"e_1_2_12_39_1","doi-asserted-by":"publisher","DOI":"10.3390\/app8020184"},{"key":"e_1_2_12_40_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.elstat.2004.09.001"},{"key":"e_1_2_12_41_1","doi-asserted-by":"publisher","DOI":"10.1039\/C8TC06302H"}],"container-title":["Advanced 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