{"data":{"id":"10.6084/m9.figshare.6504032.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6504032.v1","prefix":"10.6084","suffix":"m9.figshare.6504032.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Zeane Vieira Borges","affiliation":[],"nameIdentifiers":[]},{"name":"Poffo, Claudio Michel","nameType":"Personal","givenName":"Claudio Michel","familyName":"Poffo","affiliation":[],"nameIdentifiers":[]},{"name":"Lima, João Cardoso De","nameType":"Personal","givenName":"João Cardoso De","familyName":"Lima","affiliation":[],"nameIdentifiers":[]},{"name":"Souza, Sérgio Michielon De","nameType":"Personal","givenName":"Sérgio Michielon De","familyName":"Souza","affiliation":[],"nameIdentifiers":[]},{"name":"Trichês, Daniela Menegon","nameType":"Personal","givenName":"Daniela Menegon","familyName":"Trichês","affiliation":[],"nameIdentifiers":[]},{"name":"Biasi, Ronaldo Sérgio De","nameType":"Personal","givenName":"Ronaldo Sérgio De","familyName":"Biasi","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Structural, Thermal, Optical, and Photoacoustic Study of Mechanically Alloyed Nanocrystalline SnTe"}],"publisher":"SciELO journals","container":{},"publicationYear":2018,"subjects":[{"subject":"90499 Chemical Engineering not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Chemical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Chemical engineering","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"91207 Metals and Alloy Materials","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":"91299 Materials Engineering not elsewhere classified","subjectScheme":"FOR"}],"contributors":[],"dates":[{"date":"2018-06-13","dateType":"Created"},{"date":"2018-06-13","dateType":"Updated"},{"date":"2018","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1590/1980-5373-mr-2017-1077","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.6504032","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["2191660 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":"A nanostructured SnTe phase was produced by mechanical alloying after 2 h of milling. Part of the as-milled powder was annealed and its X-ray diffraction (XRD) pattern was recorded. The XRD patterns of the as-milled and annealed samples were refined using the Rietveld method. After annealing, partial decomposition of the SnTe phase was observed and corroborated by estimating the mean crystallite size using a Willianson-Hall plot. The Cowley-Warren parameter α SnTe CWfor the first coordination shell was calculated, showing a preference for homopolar pairs. This preference is consistent with the partial decomposition observed. According to the optical absorbance spectra, the band gap energy is inversely proportional to crystallite size, following a decaying exponential function. From the photoacoustic absorption spectroscopy measurements, the thermal diffusivity parameter and the transport properties of as-milled and annealed SnTe powder were determined.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Structural_Thermal_Optical_and_Photoacoustic_Study_of_Mechanically_Alloyed_Nanocrystalline_SnTe/6504032/1","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount"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