Magnetization‐induced optical second harmonic generation from the surface of Co‐doped rutile TiO 2 (110) | Zendy

Watanabe R. | Zendy; Yuasa M. | Zendy; Yahata Y. | Zendy; Mizutani G. | Zendy; Suzuki T. | Zendy; Segawa Y. | Zendy; Matsumoto Y. | Zendy; Yamamoto Y. | Zendy; Koinuma H. | Zendy

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Magnetization‐induced optical second harmonic generation from the surface of Co‐doped rutile TiO 2 (110)

Author(s) -

Watanabe R.,

Yuasa M.,

Yahata Y.,

Mizutani G.,

Suzuki T.,

Segawa Y.,

Matsumoto Y.,

Yamamoto Y.,

Koinuma H.

Publication year - 2008

Publication title -

surface and interface analysis

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.52

H-Index - 90

eISSN - 1096-9918

pISSN - 0142-2421

DOI - 10.1002/sia.2907

Subject(s) - rutile , magnetization , x ray photoelectron spectroscopy , hysteresis , second harmonic generation , ferromagnetism , magnetism , condensed matter physics , materials science , doping , absorption (acoustics) , kerr effect , surface layer , analytical chemistry (journal) , chemistry , layer (electronics) , magnetic field , optics , nuclear magnetic resonance , nanotechnology , physics , laser , organic chemistry , quantum mechanics , nonlinear system , chromatography , composite material

We have investigated the surface magnetism of 5 at% Co‐doped rutile TiO 2 (110) using magnetization‐induced optical second harmonic generation (MSHG) in the longitudinal Kerr configuration with the incident beam angle of 4° . MSHG is observed at both 2 ħ ω = 2.33 eV and 2 ħ ω = 4.20 eV. MSH intensity showed a hysteresis as a function of the external magnetic field for the second harmonic photon energy of 2 ħ ω = 4.20 eV at which the absorption length limits the MSHG origin to the surface layer of 10 nm due to the TiO 2 bulk. Since 5 at% Co: TiO 2 (110) is judged to have no metallic Co near the top surface by XPS, the hysteresis is attributed to a carrier‐induced ferromagnetism at the surface of this material. Copyright © 2008 John Wiley & Sons, Ltd.

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