{"data":{"id":"10.15131/shef.data.5223424","type":"dois","attributes":{"doi":"10.15131/shef.data.5223424","prefix":"10.15131","suffix":"shef.data.5223424","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":"Data for 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"}],"relatedItems":[],"sizes":["211043 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 data provided 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\u003eThe data required to reproduce each figure panel is provided in different text files. Columns are separated by a space character. The first line in each column describes the dataset.\u003cbr\u003e\u003cbr\u003eWith the added context of the paper, it should be easy to reproduce the figures. The data include original X-ray Diffraction, temperature and excitation dependent photoluminescence measurements as well as the analysed data presented in the figures of the paper.\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.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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