2017
DOI: 10.1039/c7cp05764d
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Enhanced room-temperature ferromagnetism on (In0.98−xCoxSn0.02)2O3 films: magnetic mechanism, optical and transport properties

Abstract: The effects of Co doping on the structural, optical, magnetic and transport properties of (InCoSn)O films grown by RF-magnetron sputtering were systematically investigated by theoretical and experimental techniques. The detailed structural analyses revealed that all the (InCoSn)O films possess the cubic bixbyite structure, with the substitutional Co at the In sites of the InO matrix, while some of the Co atoms form Co metal clusters. Obvious room-temperature (RT) ferromagnetic behavior was observed and the sat… Show more

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Cited by 8 publications
(4 citation statements)
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“…Combined with what we explained above, the negative MR is attributed to the formation of BMP caused by the overlap between the orbitals of electrons locally trapped by oxygen vacancy with the d shells of neighboring Cr dopants. As a result, the BMPs increase with increasing Cr content, leading to the increase in the magnitude of negative MR. Similar phenomena were also observed and calculated in previous research studies [e.g., (In 0.98– x Co x Sn 0.02 ) 2 O 3 , ZnO:Cu, La 2– x Sr x CoMnO 6 , and Zn x Fe 3– x O 4 ]. ,,,, However, excessive doping may lead to antiferromagnetic coupling between nearest neighbor’s BMPs, thus suppresses negative MR. ,, Therefore, the magnitude of negative MR is slightly smaller as the Cr content increases from 8 to 11%. Upon the polarization switching from P r + to P r – , the MR changes from negative to positive and the influences of the FE field effect on the MR is greatly enhanced with increasing Cr content.…”
Section: Resultssupporting
confidence: 87%
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“…Combined with what we explained above, the negative MR is attributed to the formation of BMP caused by the overlap between the orbitals of electrons locally trapped by oxygen vacancy with the d shells of neighboring Cr dopants. As a result, the BMPs increase with increasing Cr content, leading to the increase in the magnitude of negative MR. Similar phenomena were also observed and calculated in previous research studies [e.g., (In 0.98– x Co x Sn 0.02 ) 2 O 3 , ZnO:Cu, La 2– x Sr x CoMnO 6 , and Zn x Fe 3– x O 4 ]. ,,,, However, excessive doping may lead to antiferromagnetic coupling between nearest neighbor’s BMPs, thus suppresses negative MR. ,, Therefore, the magnitude of negative MR is slightly smaller as the Cr content increases from 8 to 11%. Upon the polarization switching from P r + to P r – , the MR changes from negative to positive and the influences of the FE field effect on the MR is greatly enhanced with increasing Cr content.…”
Section: Resultssupporting
confidence: 87%
“…For the ICO008 film and the P r – state of PMN-0.29PT, k f l ≪ 1­(Figure S8, Supporting Information), so the system is in the strongly localized regime. Such a behavior, classically observed in oxide semiconductors, could be explained by the localization phenomenon leading to variable range hopping (VRH) mechanism. Within the framework of VRH model, the temperature dependence of resistivity can be written as …”
Section: Resultsmentioning
confidence: 99%
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“…Wide bandgap oxide semiconductor films (e.g., In 2 O 3 ) are potential candidates to be used as channel materials in FeFETs. The In 2 O 3 possesses not only high conductivity and carrier mobility, and excellent transparency (>90%) in the visible region, but also relatively low carrier density (10 18 –10 19 cm −3 ), making it an idea candidate to be integrated with PMN‐ x PT.…”
Section: Introductionmentioning
confidence: 99%