Room temperature ferromagnetic behavior in the hollandite-type titanium oxide
Author(s) -
Kengo Noami,
Yuji Muraoka,
Takanori Wakita,
Masaaki Hirai,
Y. Kato,
Takayuki Muro,
Y. Tamenori,
T. Yokoya
Publication year - 2010
Publication title -
journal of applied physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.699
H-Index - 319
eISSN - 1089-7550
pISSN - 0021-8979
DOI - 10.1063/1.3369500
Subject(s) - hollandite , x ray photoelectron spectroscopy , ferromagnetism , materials science , magnetization , electrical resistivity and conductivity , valence (chemistry) , condensed matter physics , band gap , curie temperature , crystallite , analytical chemistry (journal) , chemistry , nuclear magnetic resonance , mineralogy , metallurgy , magnetic field , physics , organic chemistry , quantum mechanics , chromatography
A hollandite-type K(x)Ti(8)O(16) polycrystalline sample has been prepared and studied by magnetization, resistivity and x-ray photoelectron spectroscopy (XPS). Room temperature ferromagnetic behavior is observed in the magnetic hysteresis measurement. The sample shows a semiconductive temperature dependence in the resistivity measurement. Analysis of the Ti 2p(3/2) core-level XPS spectrum indicates that the titanium ions have a mixed valence of Ti(4+) and Ti(3+). In addition, the valence band spectrum reveals that the 3d electrons tend to localize on Ti(3+) ions in the hollandite-type TiO(2) lattice. Also, analysis of the valence band spectrum shows that the prepared sample is a wide-gap oxide with a band gap of 3.6 eV. These results indicate that the present hollandite-type K(x)Ti(8)O(16) sample can be classified as a TiO(2)-based wide-gap semiconductor with Curie temperature above room temperature. Room temperature ferromagnetism (RTFM) decreases in the sample prepared under a strong reducing gas atmosphere, accompanied with the decrease in the resistivity. The results imply that the localized 3d electrons are responsible for the RTFM of the K(x)Ti(8)O(16) sample
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