Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/100641
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dc.contributorDepartment of Electrical and Electronic Engineeringen_US
dc.contributorDepartment of Computingen_US
dc.creatorFan, Yen_US
dc.creatorXu, Yen_US
dc.creatorQiu, Men_US
dc.creatorJin, Wen_US
dc.creatorZhang, Len_US
dc.creatorLam, EYen_US
dc.creatorTsai, DPen_US
dc.creatorLei, Den_US
dc.date.accessioned2023-08-11T03:11:25Z-
dc.date.available2023-08-11T03:11:25Z-
dc.identifier.issn2192-8606en_US
dc.identifier.urihttp://hdl.handle.net/10397/100641-
dc.language.isoenen_US
dc.publisherDe Gruyteren_US
dc.rights© 2020 Yulong Fan 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 Fan, Yulong, Xu, Yunkun, Qiu, Meng, Jin, Wei, Zhang, Lei, Lam, Edmund Y., Tsai, Din Ping and Lei, Dangyuan. "Phase-controlled metasurface design via optimized genetic algorithm" Nanophotonics, vol. 9, no. 12, 2020, pp. 3931-3939 is available at https://doi.org/10.1515/nanoph-2020-0132.en_US
dc.subjectDielectric metasurfaceen_US
dc.subjectGenetic algorithmen_US
dc.subjectLight sheeten_US
dc.subjectOptical Pancharatnam-Berry phaseen_US
dc.titlePhase-controlled metasurface design via optimized genetic algorithmen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage3931en_US
dc.identifier.epage3939en_US
dc.identifier.volume9en_US
dc.identifier.issue12en_US
dc.identifier.doi10.1515/nanoph-2020-0132en_US
dcterms.abstractIn an optical Pancharatnam-Berry (PB) phase metasurface, each sub-wavelength dielectric structure of varied spatial orientation can be treated as a point source with the same amplitude yet varied relative phase. In this work, we introduce an optimized genetic algorithm (GA) method for the synthesis of one-dimensional (1D) PB phase-controlled dielectric metasurfaces by seeking for optimized phase profile solutions, which differs from previously reported amplitude-controlled GA method only applicable to generate transverse optical modes with plasmonic metasurfaces. The GA-optimized phase profiles can be readily used to construct dielectric metasurfaces with improved functionalities. The loop of phase-controlled GA consists of initialization, random mutation, screened evolution, and duplication. Here random mutation is realized by changing the phase of each unit cell, and this process should be efficient to obtain enough mutations to drive the whole GA process under supervision of appropriate mutation boundary. A well-chosen fitness function ensures the right direction of screened evolution, and the duplication process guarantees an equilibrated number of generated light patterns. Importantly, we optimize the GA loop by introducing a multi-step hierarchical mutation process to break local optimum limits. We demonstrate the validity of our optimized GA method by generating longitudinal optical modes (i. e., non-diffractive light sheets) with 1D PB phase dielectric metasurfaces having non-analytical counter-intuitive phase profiles. The produced large-area, long-distance light sheets could be used for realizing high-speed, low-noise light-sheet microscopy. Additionally, a simplified 3D light pattern generated by a 2D PB phase metasurface further reveals the potential of our optimized GA method for manipulating truly 3D light fields.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationNanophotonics, Sept. 2020, v. 9, no. 12, p. 3931-3939en_US
dcterms.isPartOfNanophotonicsen_US
dcterms.issued2020-09-
dc.identifier.scopus2-s2.0-85093644497-
dc.identifier.eissn2192-8614en_US
dc.description.validate202307 bckwen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberEE-0748-
dc.description.fundingSourceOthersen_US
dc.description.fundingTextCity University of Hong Kong; Hong Kong Polytechnic University; Shenzhen Science and Technology Innovation Commissionen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS43054919-
dc.description.oaCategoryCCen_US
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