{"data":{"id":"10.6084/m9.figshare.c.4005961","type":"dois","attributes":{"doi":"10.6084/m9.figshare.c.4005961","prefix":"10.6084","suffix":"m9.figshare.c.4005961","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Vaughn, Israel","nameType":"Personal","givenName":"Israel","familyName":"Vaughn","affiliation":[],"nameIdentifiers":[]},{"name":"Alenin, Andrey","nameType":"Personal","givenName":"Andrey","familyName":"Alenin","affiliation":[],"nameIdentifiers":[]},{"name":"J. Scott Tyo","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Channeled spatio-temporal Stokes polarimeters"}],"publisher":"Figshare","container":{},"publicationYear":2018,"subjects":[{"subject":"90605 Photodetectors, Optical Sensors and Solar Cells","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)"},{"subject":"Instrumentation, Techniques, and Astronomical Observations"},{"subject":"111302 Optical Technology","subjectScheme":"FOR"},{"subject":"FOS: Clinical medicine","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2018-02-15","dateType":"Created"},{"date":"2018-06-01","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.43.002768","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":[],"version":null,"rightsList":[{"rights":"CC BY 4.0","rightsUri":"https://creativecommons.org/licenses/by/4.0"}],"descriptions":[{"description":"We present the analysis and design of spatio-temporal channeled Stokes polarimeters. We extend our recent work on optimal pixelated polarizer arrays by utilizing temporal carrier generation, resulting in polarimeters which achieve super-resolution via the tradeoff between spatial bandwidth and temporal bandwidth. Utilizing the channel space description, we present a linear Stokes and two full-Stokes imaging polarimeter designs which have the potential to operate at the full frame rate of the imaging sensor of the system by using a hybrid spatio-temporal carrier design. If the objects are not spatially bandlimited, then the achievable temporal bandwidth is more difficult to analyze, however a spatio-temporal tradeoff still exists.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://figshare.com/collections/Channeled_spatio-temporal_Stokes_polarimeters/4005961","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":"2018-06-01T20:27:22.000Z","registered":"2018-06-01T20:27:22.000Z","published":"2018","updated":"2024-12-12T12:28:05.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.c.4005961","type":"media"}},"references":{"data":[{"id":"10.1364/ol.43.002768","type":"dois"}]},"citations":{"data":[]},"parts":{"data":[]},"partOf":{"data":[]},"versi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