{"data":{"id":"10.4121/13606598","type":"dois","attributes":{"doi":"10.4121/13606598","prefix":"10.4121","suffix":"13606598","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Korzun, K. (Ksenia)","givenName":"K. (Ksenia)","familyName":"Korzun","nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0001-6124-6168","nameIdentifierScheme":"ORCID"}],"affiliation":[]},{"name":"Castellanos Gonzalez, Gabriel","givenName":"Gabriel","familyName":"Castellanos Gonzalez","affiliation":[],"nameIdentifiers":[]},{"name":"Boer, Dick K.G. de","givenName":"Dick K.G. de","familyName":"Boer","affiliation":[],"nameIdentifiers":[]},{"name":"Gomez Rivas, Jaime","givenName":"Jaime","familyName":"Gomez Rivas","nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0002-8038-0968","nameIdentifierScheme":"ORCID"}],"affiliation":[]},{"name":"Haverkort, Jos","givenName":"Jos","familyName":"Haverkort","nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-3051-673X","nameIdentifierScheme":"ORCID"}],"affiliation":[]}],"titles":[{"title":"Dataset for Nanowire solar cell above the radiative limit"}],"publisher":"4TU.ResearchData","container":{},"publicationYear":2021,"subjects":[{"subject":"Renewable Energy"},{"subject":"Optical Physics"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Condensed Matter Physics"}],"contributors":[],"dates":[{"date":"2021-01-20","dateType":"Created"},{"date":"2023-06-02","dateType":"Updated"},{"date":"2021-01-20","dateType":"Issued"}],"language":null,"types":{"ris":"COMP","bibtex":"misc","citeproc":"article","schemaOrg":"SoftwareSourceCode","resourceType":"Software","resourceTypeGeneral":"Software"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1002/adom.202001636","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["4329328 Bytes"],"formats":[],"version":"1","rightsList":[{"rights":"Creative Commons Zero v1.0 Universal","rightsUri":"https://creativecommons.org/publicdomain/zero/1.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc0-1.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"A lossless\nsolar cell operating at the Shockley-Queisser limit generates an open circuit\nvoltage (V\u003csub\u003eoc\u003c/sub\u003e) equal to the radiative limit. At V\u003csub\u003eoc\u003c/sub\u003e, the highly\ndirectional beam of photons from the sun is absorbed and subsequently externally\nre-emitted into a 4π solid angle, providing a large photon entropy loss. A\nsolar cell can beat the Shockley-Queisser limit and approach the 46.7% ultimate\nlimit by decreasing the output solid angle of the light emission at open\ncircuit conditions. Here, we present a\ndesign for an InP single nanowire solar cell capable to operate 159 mV above\nthe radiative limit. We first optimize the spontaneous emission factor (b-factor in the dataset) into a\nguided mode of the nanowire towards 68%. We subsequently launch a guided mode at\nthe bottom straight part of the tapered nanowire yielding a photon escape\nprobability of 81% for a tapering angle of θ=1.2 degrees\n \n \n \n \n \n \n \n \n \n \n \n \n \n \n \n \n \n\n \n and a top facet with a radius of 83 nm (transmission part of the dataset). When\nassuming homogeneous light emission along the nanowire, an outcoupling\nefficiency of 42% of the emitted light is obtained. The final optimization is\nthe reduction of the emission cone towards 0.011 sr by focusing the guided mode with an\nexternal lens (lens part of the dataset).\u003cbr\u003e\u003cbr\u003e","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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