Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/96598
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dc.contributorDepartment of Mechanical Engineering-
dc.creatorChen, Yen_US
dc.creatorLan, Zen_US
dc.creatorZhu, Jen_US
dc.date.accessioned2022-12-07T02:55:33Z-
dc.date.available2022-12-07T02:55:33Z-
dc.identifier.issn2192-8606en_US
dc.identifier.urihttp://hdl.handle.net/10397/96598-
dc.language.isoenen_US
dc.publisherDe Gruyteren_US
dc.rights© 2022 Yafeng Chen et al., published by De Gruyter. This work is licensed under the Creative Commons Attribution 4.0 International License (https://creativecommons.org/licenses/by/4.0/).en_US
dc.rightsThe following publication Chen, Y., Lan, Z., & Zhu, J. (2022). Second-order topological phases in C 4v-symmetric photonic crystals beyond the two-dimensional Su-Schrieffer–Heeger model. Nanophotonics, 11(7), 1345-1354 is available at https://doi.org/10.1515/nanoph-2021-0762.en_US
dc.subjectInverse designen_US
dc.subjectOdd-order band gapen_US
dc.subjectPhotonic crystalen_US
dc.subjectSecond-order topological insulatorsen_US
dc.titleSecond-order topological phases in C4v-symmetric photonic crystals beyond the two-dimensional Su-Schrieffer–Heeger modelen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage1345en_US
dc.identifier.epage1354en_US
dc.identifier.volume11en_US
dc.identifier.issue7en_US
dc.identifier.doi10.1515/nanoph-2021-0762en_US
dcterms.abstractSecond-order photonic topological insulators (SPTIs) with topologically protected corner states provide a unique platform for realizing the robust manipulation of light in lower dimensions. Previous SPTIs proposed in C4v-symmetric lattices are mainly based on the two-dimensional (2D) Su-Schrieffer-Heeger (SSH) model consisting of an even number of sites in the unit cell. Moreover, second-order topological phases within high-order band gaps are rarely explored. Here, we propose a new principle of SPTIs beyond the 2D SSH model, which is realized in C4v-symmetric lattices consisting of an odd number of sites in the unit cell. The midgap-gap-ratios of these odd-order band gaps, from the first-order to the nineteenth-order with step of two-order, are maximized by the method of topology optimization. Second-order topological phases are successfully created within these sizeable band gaps and highly localized corner states are observed. Our work offers a new route for exploring high-order topological states in photonics and other classical systems.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationNanophotonics, Mar. 2022, v. 11, no. 7, p. 1345-1354en_US
dcterms.isPartOfNanophotonicsen_US
dcterms.issued2022-03-
dc.identifier.scopus2-s2.0-85126058416-
dc.identifier.eissn2192-8614en_US
dc.description.validate202212 bckw-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_Scopus/WOS-
dc.description.pubStatusPublisheden_US
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