{"data":{"id":"10.6084/m9.figshare.6857339","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6857339","prefix":"10.6084","suffix":"m9.figshare.6857339","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Bonifacich, Federico Guillermo","nameType":"Personal","givenName":"Federico Guillermo","familyName":"Bonifacich","affiliation":[],"nameIdentifiers":[]},{"name":"Lambri, Osvaldo Agustín","nameType":"Personal","givenName":"Osvaldo Agustín","familyName":"Lambri","affiliation":[],"nameIdentifiers":[]},{"name":"Pérez-Landazábal, José Ignacio","nameType":"Personal","givenName":"José Ignacio","familyName":"Pérez-Landazábal","affiliation":[],"nameIdentifiers":[]},{"name":"Recarte, Vicente","nameType":"Personal","givenName":"Vicente","familyName":"Recarte","affiliation":[],"nameIdentifiers":[]},{"name":"Gargicevich, Damián","nameType":"Personal","givenName":"Damián","familyName":"Gargicevich","affiliation":[],"nameIdentifiers":[]},{"name":"Zelada, Griselda Irene","nameType":"Personal","givenName":"Griselda Irene","familyName":"Zelada","affiliation":[],"nameIdentifiers":[]},{"name":"Mocellini, Ricardo Raúl","nameType":"Personal","givenName":"Ricardo Raúl","familyName":"Mocellini","affiliation":[],"nameIdentifiers":[]},{"name":"Sánchez-Alarcos, Vicente","nameType":"Personal","givenName":"Vicente","familyName":"Sánchez-Alarcos","affiliation":[],"nameIdentifiers":[]},{"name":"Marenzana, Aldo","nameType":"Personal","givenName":"Aldo","familyName":"Marenzana","affiliation":[],"nameIdentifiers":[]},{"name":"Plazaola, Fernando","nameType":"Personal","givenName":"Fernando","familyName":"Plazaola","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Study of the martensitic transition in Ni-Mn-Sn-Ti ferromagnetic shape memory alloys"}],"publisher":"SciELO journals","container":{},"publicationYear":2018,"subjects":[{"subject":"90502 Construction Engineering","subjectScheme":"FOR"},{"subject":"FOS: Civil engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Civil 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":"2018-07-25","dateType":"Created"},{"date":"2018-07-25","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/s1517-707620180002.0379","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["2221258 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":"ABSTRACT In the present work, mechanical spectroscopy measurements as a function of temperature and strain have been performed in (at.%) Ni50Mn37Sn13-xTix (x=0, 0.5 and 2) ferromagnetic shape memory alloys in order both to study martensitic transition phenomenon and also to determine its temperature of appearance. For mechanical spectroscopy measurements, a five elements piezoelectric device recently developed has been used. In addition, other characterization techniques as, differential thermal analysis and superconducting quantum interference magnetic spectroscopy, were also used. Besides, relaxation processes near the martensitic transition temperature have been also observed.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Study_of_the_martensitic_transition_in_Ni-Mn-Sn-Ti_ferromagnetic_shape_memory_alloys/6857339","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":1,"citationCount":0,"citationsOverTime":[],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2018-07-25T02:47:43.000Z","registered":"2018-07-25T02:48:55.000Z","published":"2018","updated":"2020-08-28T16:25:22.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.6857339","type":"media"}},"references":{"data":[{"id":"10.1590/s1517-707620180002.0379","type":"dois"}]},"citations":{"data":[]},"parts":{"data":[]},"partOf":{"data":[]},"versions":{"data":[]},"versionOf":{"data":[]}}}}