{"data":{"id":"10.4121/6d527ad0-df6b-4df5-a0a0-a8b62ef1e213","type":"dois","attributes":{"doi":"10.4121/6d527ad0-df6b-4df5-a0a0-a8b62ef1e213","prefix":"10.4121","suffix":"6d527ad0-df6b-4df5-a0a0-a8b62ef1e213","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Berghuis, Anton Matthijs","nameType":"Personal","givenName":"Anton Matthijs","familyName":"Berghuis","nameIdentifiers":[{"nameIdentifier":"0000-0002-1896-7119","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Schneider, Tobias","givenName":"Tobias","familyName":"Schneider","affiliation":[],"nameIdentifiers":[]},{"name":"Schumacher, Stefan","nameType":"Personal","givenName":"Stefan","familyName":"Schumacher","nameIdentifiers":[{"nameIdentifier":"0000-0003-4042-4951","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Murai, Shunsuke","nameType":"Personal","givenName":"Shunsuke","familyName":"Murai","nameIdentifiers":[{"nameIdentifier":"0000-0002-4597-973X","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Pura, Jose Luis","nameType":"Personal","givenName":"Jose Luis","familyName":"Pura","nameIdentifiers":[{"nameIdentifier":"0000-0002-8272-527X","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Sánchez-Gil, José A.","nameType":"Personal","givenName":"José A.","familyName":"Sánchez-Gil","nameIdentifiers":[{"nameIdentifier":"0000-0002-5370-3717","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Ma, Xuekai","nameType":"Personal","givenName":"Xuekai","familyName":"Ma","nameIdentifiers":[{"nameIdentifier":"0000-0002-6659-4134","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Gómez Rivas, Jaime","nameType":"Personal","givenName":"Jaime","familyName":"Gómez Rivas","nameIdentifiers":[{"nameIdentifier":"0000-0002-8038-0968","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]}],"titles":[{"title":"Data underlying the publication: Optical Control of the Polarization State of a Polariton Condensate in a Bound State in the Continuum"}],"publisher":"4TU.ResearchData","container":{},"publicationYear":2025,"subjects":[{"subject":"Condensed Matter Physics","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0204"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Optical Physics","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0205"},{"subject":"Physical Sciences","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"02"},{"subject":"Metasurfaces"},{"subject":"Bound State in the Continuum"},{"subject":"Polariton condensation"},{"subject":"Laser"}],"contributors":[{"name":"TU Eindhoven, Department of Applied Physics and Science Education","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]}],"dates":[{"date":"2025-10-24","dateType":"Issued"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsVersionOf","relatedIdentifier":"10.4121/6d527ad0-df6b-4df5-a0a0-a8b62ef1e213.v1","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":["csv, Excell, tiff. python and matlab"],"version":"1","rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"The data underlying all figures of the associated manuscript about polarization control in a polariton laser. We investigated the emission properties of a polariton condensate under different pump geometries. We show that we can control the polarization of the condensate above lasing threshold. The core part of the data consists of images of an imaging spectrometer of a Fourier microscope showing angle resolved emission spectra (theta_x vs wavelength and theta_x vs theta_y) of the sample under different excitation fluences and geometries. Besides that there is the polarization data of the emission, data from RCWA simulations and Gross Pitaevski simulations.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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