{"data":{"id":"10.6084/m9.figshare.6802460.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6802460.v1","prefix":"10.6084","suffix":"m9.figshare.6802460.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Aghazadeh, Mustafa","nameType":"Personal","givenName":"Mustafa","familyName":"Aghazadeh","affiliation":[],"nameIdentifiers":[]},{"name":"Karimzadeh, Isa","nameType":"Personal","givenName":"Isa","familyName":"Karimzadeh","affiliation":[],"nameIdentifiers":[]},{"name":"Maragheh, Mohammad Ghannadi","nameType":"Personal","givenName":"Mohammad Ghannadi","familyName":"Maragheh","affiliation":[],"nameIdentifiers":[]},{"name":"Ganjali, Mohammad Reza","nameType":"Personal","givenName":"Mohammad Reza","familyName":"Ganjali","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Enhancing the Supercapacitive and Superparamagnetic Performances of Iron Oxide Nanoparticles through Yttrium Cations Electro-chemical Doping"}],"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":"2018-07-11","dateType":"Created"},{"date":"2018-07-11","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-2018-0094","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.6802460","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["1965476 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 one-pot electrosynthesis platform is reported for fabrication of Y3+ doped iron oxide nanoparticles (Y-IONPs). In this procedure, Y-IONPs are electro-deposited from an additive-free aqueous solution of iron(III) nitrate, iron(II) chloride and yttrium chloride. The analysis data provided by X-ray diffraction (XRD), field emission electron microscopy (FE-SEM) and energy-dispersive X-ray (EDX) confirmed that the deposited Y-IONPs sample is composed of magnetite nanoparticles (size≈20nm) doped with about 10wt% Y3+ cations. The performance of the prepared Y-IONPs as supercapacitor electrode material was studied using cyclic voltammetry (CV) and galvanostat charge-discharge (GCD) tests. The obtained electrochemical data showed that Y-IONPs provide SCs as high as 190.3 and 138.9 F g−1 at the discharge loads of 0.25 and 1 A g−1, respectively, and capacity retentions of 95.9% and 88.5% after 2000 GCD cycling. Furthermore, the results of vibrating sample magnetometer measurements confirmed better superparamagnetic behavior of Y-IONPs (Mr=0.32 emu g-1 and HCi= 6.31 G) as compared with pure IONPs (Mr=0.95 emu g-1 and HCi= 14.62 G) resulting from their lower Mr and Hci values. Based on the obtained results, the developed electro-synthesis method was introduced as a facile procedure for the preparation of high performance metal ion doped magnetite nanoparticles.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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