{"data":{"id":"10.6084/m9.figshare.c.4051997","type":"dois","attributes":{"doi":"10.6084/m9.figshare.c.4051997","prefix":"10.6084","suffix":"m9.figshare.c.4051997","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Yingjie Liu","affiliation":[],"nameIdentifiers":[]},{"name":"Wenzhao Sun","affiliation":[],"nameIdentifiers":[]},{"name":"Hucheng Xie","affiliation":[],"nameIdentifiers":[]},{"name":"Zhang, Nan","nameType":"Personal","givenName":"Nan","familyName":"Zhang","affiliation":[],"nameIdentifiers":[]},{"name":"Xu, Ke","nameType":"Personal","givenName":"Ke","familyName":"Xu","affiliation":[],"nameIdentifiers":[]},{"name":"Yao, Yong","nameType":"Personal","givenName":"Yong","familyName":"Yao","affiliation":[],"nameIdentifiers":[]},{"name":"Shumin Xiao","affiliation":[],"nameIdentifiers":[]},{"name":"Qinghai Song","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Very sharp adiabatic bends based on inverse design"}],"publisher":"Figshare","container":{},"publicationYear":2018,"subjects":[{"subject":"90606 Photonics and Electro-Optical Engineering (excl. Communications)","subjectScheme":"FOR"},{"subject":"FOS: Electrical engineering, electronic engineering, information engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2018-03-29","dateType":"Created"},{"date":"2018-05-15","dateType":"Updated"},{"date":"2018","dateType":"Issued"}],"language":null,"types":{"ris":"GEN","bibtex":"misc","citeproc":"article","schemaOrg":"Collection","resourceType":"Collection","resourceTypeGeneral":"Collection"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1364/ol.43.002482","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[{"rights":"CC BY 4.0","rightsUri":"https://creativecommons.org/licenses/by/4.0"}],"descriptions":[{"description":"Very sharp 90°micro-bends for adiabatic optical wave propagation in multimode waveguides are demonstrated by inverse design method and the devices are fabricated on silicon-on-insulator platform. The compact bending structures are based on digital waveguide metastructures with footprints as small as 2.6×2.6 μm². For waveguides width of 2μm and bending radius of only 1 μm, the TE00 mode is able to turn around the sharp corner with 1dB loss and \u0026gt;20 dB suppression ratio to higher order modes. The transmission spectra of the devices are measured with ~1 dB loss over 40 nm bandwidth which are consistent with the numerical simulations.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.com/collections/Very_sharp_adiabatic_bends_based_on_inverse_design/4051997","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"api","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":1,"citationCount":0,"citationsOverTime":[],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2018-05-15T18:08:16.000Z","registered":"2018-05-15T18:08:17.000Z","published":"2018","updated":"2024-12-12T11:36:43.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.c.4051997","type":"media"}},"references":{"data":[{"id":"10.1364/ol.43.002482","t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