{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,9,25]],"date-time":"2026-09-25T07:58:31Z","timestamp":1790323111524,"version":"4.1.0"},"reference-count":56,"publisher":"Wiley","issue":"18","license":[{"start":{"date-parts":[[2026,9,22]],"date-time":"2026-09-22T00:00:00Z","timestamp":1790035200000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/creativecommons.org\/licenses\/by\/4.0\/"},{"start":{"date-parts":[[2026,9,22]],"date-time":"2026-09-22T00:00:00Z","timestamp":1790035200000},"content-version":"tdm","delay-in-days":0,"URL":"http:\/\/doi.wiley.com\/10.1002\/tdm_license_1.1"}],"funder":[{"DOI":"10.13039\/501100001809","name":"National Natural Science Foundation of China","doi-asserted-by":"publisher","award":["12604483"],"award-info":[{"award-number":["12604483"]}],"id":[{"id":"10.13039\/501100001809","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["onlinelibrary.wiley.com"],"crossmark-restriction":true},"short-container-title":["Nanophotonics"],"published-print":{"date-parts":[[2026,9,25]]},"abstract":"<jats:title>ABSTRACT<\/jats:title>\n                  <jats:p>Exciton\u2013polaritons arising from strong light\u2013matter coupling are key enablers of quantum coherent phenomena, whereas large Rabi splitting is critical for ensuring their robustness and stability. However, existing microcavity photonic modes rarely combine low radiative dissipation with strong field confinement, thereby limiting large splitting strong coupling, particularly in the few\u2010exciton regime. Here, we design a metal\u2013dielectric hybrid cavity in which coherent hybridization among plasmon resonances, magnetic quadrupole modes, and anapole states gives rise to a plasmon\u2010enhanced hybrid anapole state (HAS) featuring narrow linewidths (54\u00a0meV) and strong field localization (180\u2010fold). Based on the plasmon\u2010enhanced HAS, we realize both HAS\u2013exciton and HAS\u2013plasmon polaritons and further demonstrate HAS\u2013plasmon\u2013exciton triplex polaritons enabled by multichannel radiative coupling. The ternary system achieves a Rabi splitting of 330\u00a0meV, six times larger than the binary case, with a reduced effective exciton number of 6205 based on a characteristic excitonic volume, significantly lower than values reported for the dielectric\u2010exciton systems under the same volume\u2010based estimation procedure. A three\u2010coupled oscillator model elucidates the light\u2013matter interaction mechanism, providing a new pathway to efficient room\u2010temperature strong coupling and a design guide for high\u2010performance dielectric\u2010cavity\u2010based polariton devices.<\/jats:p>","DOI":"10.1002\/nap2.70296","type":"journal-article","created":{"date-parts":[[2026,9,22]],"date-time":"2026-09-22T08:47:12Z","timestamp":1790066832000},"update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":0,"title":["Large Rabi Splitting Driven by Plasmon\u2010Enhanced Hybrid Anapole States in Si\u2013Au\u2013WSe\n                    <sub>2<\/sub>\n                    Heterostructures"],"prefix":"10.1002","volume":"15","author":[{"given":"Yanhui","family":"Deng","sequence":"first","affiliation":[{"name":"Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Center for Intense Laser Application Technology, and College of Engineering Physics Shenzhen Technology University  Shenzhen China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Mingyang","family":"Yu","sequence":"additional","affiliation":[{"name":"Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Center for Intense Laser Application Technology, and College of Engineering Physics Shenzhen Technology University  Shenzhen China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Xizhen","family":"Xing","sequence":"additional","affiliation":[{"name":"Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Center for Intense Laser Application Technology, and College of Engineering Physics Shenzhen Technology University  Shenzhen China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Chenxi","family":"Zhao","sequence":"additional","affiliation":[{"name":"Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Center for Intense Laser Application Technology, and College of Engineering Physics Shenzhen Technology University  Shenzhen China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Tianyu","family":"Yang","sequence":"additional","affiliation":[{"name":"Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Center for Intense Laser Application Technology, and College of Engineering Physics Shenzhen Technology University  Shenzhen China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0009-0009-7908-3083","authenticated-orcid":false,"given":"Yujie","family":"Ma","sequence":"additional","affiliation":[{"name":"Shenzhen Key Laboratory of Ultraintense Laser and Advanced Material Technology, Center for Intense Laser Application Technology, and College of Engineering Physics Shenzhen Technology University  Shenzhen China"},{"name":"Guangdong Engineering Technology Research Center for High\u2010Power Ultrafast Laser and X\u2010Ray Equipment  Shenzhen China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-4341-3097","authenticated-orcid":false,"given":"Zhang\u2010Kai","family":"Zhou","sequence":"additional","affiliation":[{"name":"State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics Sun Yat\u2010Sen University  Guangzhou China"},{"name":"Quantum Science Center of Guangdong\u2013Hong Kong\u2013Macao Greater Bay Area (Guangdong)  Shenzhen China"}],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"311","published-online":{"date-parts":[[2026,9,22]]},"reference":[{"key":"e_1_2_9_2_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsphotonics.7b00674"},{"key":"e_1_2_9_3_1","doi-asserted-by":"publisher","DOI":"10.1038\/s42254\u2010022\u201000447\u20101"},{"key":"e_1_2_9_4_1","doi-asserted-by":"publisher","DOI":"10.1117\/1.ap.7.1.016003"},{"key":"e_1_2_9_5_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.pquantelec.2019.04.002"},{"key":"e_1_2_9_6_1","doi-asserted-by":"publisher","DOI":"10.1088\/0034\u20104885\/78\/1\/013901"},{"key":"e_1_2_9_7_1","doi-asserted-by":"publisher","DOI":"10.1088\/1361\u20106463\/ac3fdf"},{"key":"e_1_2_9_8_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41467\u2010024\u201047669\u20108"},{"key":"e_1_2_9_9_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41586\u2010022\u201004583\u20107"},{"key":"e_1_2_9_10_1","doi-asserted-by":"publisher","DOI":"10.1038\/nphoton.2012.340"},{"key":"e_1_2_9_11_1","doi-asserted-by":"publisher","DOI":"10.1038\/nphoton.2012.181"},{"key":"e_1_2_9_12_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41586\u2010019\u20101709\u2010y"},{"key":"e_1_2_9_13_1","doi-asserted-by":"publisher","DOI":"10.1126\/sciadv.abj8905"},{"key":"e_1_2_9_14_1","doi-asserted-by":"publisher","DOI":"10.1103\/jk6y\u201055xp"},{"key":"e_1_2_9_15_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41567\u2010025\u201003115\u20100"},{"key":"e_1_2_9_16_1","doi-asserted-by":"publisher","DOI":"10.1126\/science.aaq0327"},{"key":"e_1_2_9_17_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevlett.118.237401"},{"key":"e_1_2_9_18_1","doi-asserted-by":"publisher","DOI":"10.1002\/nap2.70088"},{"key":"e_1_2_9_19_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevlett.111.216805"},{"key":"e_1_2_9_20_1","doi-asserted-by":"publisher","DOI":"10.29026\/oea.2019.190008"},{"key":"e_1_2_9_21_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41578\u2010022\u201000440\u20101"},{"key":"e_1_2_9_22_1","doi-asserted-by":"publisher","DOI":"10.1021\/acs.nanolett.9b00484"},{"key":"e_1_2_9_23_1","doi-asserted-by":"publisher","DOI":"10.1021\/acs.nanolett.1c04360"},{"key":"e_1_2_9_24_1","doi-asserted-by":"publisher","DOI":"10.1021\/acs.nanolett.7b01176"},{"key":"e_1_2_9_25_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41467\u2010017\u201001398\u20103"},{"key":"e_1_2_9_26_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevlett.130.143601"},{"key":"e_1_2_9_27_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevlett.133.053801"},{"key":"e_1_2_9_28_1","doi-asserted-by":"publisher","DOI":"10.1515\/nanoph\u20102019\u20100371"},{"key":"e_1_2_9_29_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsnano.5c01972"},{"key":"e_1_2_9_30_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevb.105.195425"},{"key":"e_1_2_9_31_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.mtchem.2020.100254"},{"key":"e_1_2_9_32_1","doi-asserted-by":"publisher","DOI":"10.1038\/s41565\u2010019\u20100442\u2010x"},{"key":"e_1_2_9_33_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevb.111.155429"},{"key":"e_1_2_9_34_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevb.98.165419"},{"key":"e_1_2_9_35_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevb.109.195425"},{"key":"e_1_2_9_36_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsphotonics.0c01470"},{"key":"e_1_2_9_37_1","doi-asserted-by":"publisher","DOI":"10.1021\/acs.jpclett.9b01844"},{"key":"e_1_2_9_38_1","doi-asserted-by":"publisher","DOI":"10.1103\/physrevb.107.075415"},{"key":"e_1_2_9_39_1","doi-asserted-by":"publisher","DOI":"10.1007\/s11433\u2010023\u20102183\u20105"},{"key":"e_1_2_9_40_1","doi-asserted-by":"publisher","DOI":"10.1364\/ol.584009"},{"key":"e_1_2_9_41_1","doi-asserted-by":"publisher","DOI":"10.1364\/OL.560479"},{"key":"e_1_2_9_42_1","doi-asserted-by":"publisher","DOI":"10.1088\/1361\u20106463\/ad316a"},{"key":"e_1_2_9_43_1","doi-asserted-by":"publisher","DOI":"10.1364\/oe.427141"},{"key":"e_1_2_9_44_1","doi-asserted-by":"publisher","DOI":"10.1364\/prj.453099"},{"key":"e_1_2_9_45_1","doi-asserted-by":"publisher","DOI":"10.1103\/PhysRevB.98.161113"},{"key":"e_1_2_9_46_1","doi-asserted-by":"publisher","DOI":"10.1103\/xsdc\u2010jj4t"},{"key":"e_1_2_9_47_1","doi-asserted-by":"publisher","DOI":"10.1007\/s40843\u2010021\u20101686\u20102"},{"key":"e_1_2_9_48_1","doi-asserted-by":"publisher","DOI":"10.1088\/1367\u20102630\/abde6c"},{"key":"e_1_2_9_49_1","doi-asserted-by":"publisher","DOI":"10.1016\/j.optcom.2017.08.064"},{"key":"e_1_2_9_50_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsphotonics.8b01194"},{"key":"e_1_2_9_51_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsphotonics.2c00433"},{"key":"e_1_2_9_52_1","doi-asserted-by":"publisher","DOI":"10.1364\/prj.514576"},{"key":"e_1_2_9_53_1","doi-asserted-by":"publisher","DOI":"10.1021\/acsanm.4c06648"},{"key":"e_1_2_9_54_1","doi-asserted-by":"publisher","DOI":"10.1021\/acs.nanolett.2c03385"},{"key":"e_1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