Room-temperature ferromagnetism in carbon- and nitrogen-doped rutile TiO sub(2)

Marked room-temperature ferromagnetism (RTFM) was obtained in carbon- and nitrogen-doped rutile \(\hbox {TiO}_2\) powders. X-ray photoelectron spectroscopy measurements revealed the co-existence of considerable densities of states near the Fermi level ( \(E_{\rm F}\) ) and oxygen vacancies primarily...

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Published inApplied physics. A, Materials science & processing Vol. 118; no. 2; pp. 725 - 731
Main Authors Wang, Jia-Bin, Wu, Kuei-Ching, Mi, Jyun-Wei, Luo, Chih-Wei, Wu, Kaung-Hsiung, Uen, Tzeng-Ming, Lin, Jiunn-Yuan, Juang, Jenh-Yih, Liu, Shiu-Jen
Format Journal Article
LanguageEnglish
Published 01.02.2015
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Summary:Marked room-temperature ferromagnetism (RTFM) was obtained in carbon- and nitrogen-doped rutile \(\hbox {TiO}_2\) powders. X-ray photoelectron spectroscopy measurements revealed the co-existence of considerable densities of states near the Fermi level ( \(E_{\rm F}\) ) and oxygen vacancies primarily induced by C- and N-doping. Density functional theory calculations showed that the local moments responsible for the observed RTFM in N-doped \(\hbox {TiO}_2\) were primarily attributed to the partially populated, spin-polarized Ti \(3d\) band. In addition to the unfilled Ti \(3d\) band, the spin splitting in C \(2p\) states near \(E_{\rm F}\) in C-doped \(\hbox {TiO}_2\) , which may be induced by the \(p-p\) interaction between the C impurities and neighboring oxygen ions, results in Stoner band-splitting-type ferromagnetism.
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ISSN:0947-8396
1432-0630
DOI:10.1007/s00339-014-8788-2