{"data":{"id":"10.15131/shef.data.5223535.v1","type":"dois","attributes":{"doi":"10.15131/shef.data.5223535.v1","prefix":"10.15131","suffix":"shef.data.5223535.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Trapalis, Aristotelis","nameType":"Personal","givenName":"Aristotelis","familyName":"Trapalis","affiliation":[],"nameIdentifiers":[{"schemeUri":"https://orcid.org","nameIdentifier":"https://orcid.org/0000-0003-4887-7058","nameIdentifierScheme":"ORCID"}]}],"titles":[{"title":"Figures in paper 'Temperature dependence of the band gap of zinc nitride observed in photoluminescence measurements'"}],"publisher":"The University of Sheffield","container":{},"publicationYear":2017,"subjects":[{"subject":"91203 Compound Semiconductors","subjectScheme":"FOR"},{"subject":"FOS: Materials engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Materials engineering","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Crystallography"},{"subject":"30303 Optical Properties of Materials","subjectScheme":"FOR"},{"subject":"FOS: Chemical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Chemical sciences","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2017-10-06","dateType":"Created"},{"date":"2021-04-22","dateType":"Updated"},{"date":"2017","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1063/1.4997153","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.15131/shef.data.5223535","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["561998 Bytes"],"formats":[],"version":null,"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 figures included here are related to the publication:\u003cbr\u003e\"Temperature dependence of the band gap of zinc nitride observed in photoluminescence measurements\".\u003cbr\u003eAppl. Phys. Lett. 111, 122105 (2017); doi: http://dx.doi.org/10.1063/1.4997153\u003cbr\u003e\u003cbr\u003eThe study reported in this paper was funded by the EPSRC (Fund code EP/M507611/1) and Johnson Matthey PLC. The financial support by these parties is highly appreciated.\u003cbr\u003e\u003cbr\u003e\u003cb\u003eFigure 1:\u003c/b\u003e XRD pattern of a sample grown at 150 °C. Inset: SEM image of the same sample.\u003cbr\u003e\u003cb\u003e\u003cbr\u003eFigure 2:\u003c/b\u003e Temperature dependent PL of a sample shortly after growth. The excitation power for these measurements was set to 30 mW.\u003cbr\u003e\u003cbr\u003e\u003cb\u003eFigure 3:\u003c/b\u003e (a) Temperature dependent PL of the zinc nitride sample after prolonged exposure to ambient. (b) Comparison of the high-energy bands of the same sample before (solid) and after (dashed) prolonged exposure to ambient.\u003cbr\u003e\u003cbr\u003e\u003cb\u003eFigure 4:\u003c/b\u003e PL spectra of bands A and B at (a) 3.7 and (b) 294 K at different excitation powers. (c) Peak intensities and (d) emission energies of band A at 294 K (●) and bands A (▼) and B (▲) at 3.7 K as a function of excitation power. The spectra in (a) have been normalised at the maximum intensity of band A.\u003cbr\u003e\u003cbr\u003e\u003cb\u003eFigure 5:\u003c/b\u003e Temperature dependence of (a) relative integrated intensities (I/I0) and (b) the emission energies of band A at an excitation power of 100 mW (●) and bands A (▼) and B (▲) at an excitation power of 1 mW.\u003cbr\u003e","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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