2017年第64回応用物理学会春季学術講演会

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一般セッション(口頭講演)

6 薄膜・表面 » 6.6 プローブ顕微鏡

[14a-414-1~8] 6.6 プローブ顕微鏡

6.6と12.2のコードシェアセッションあり

2017年3月14日(火) 09:30 〜 11:30 414 (414+415)

武内 修(筑波大)

09:45 〜 10:00

[14a-414-2] Investigation of local surface potential induced by atomic dipole moment on TiO2(110) surface by Kelvin Probe Force Microscopy

〇(D)Zhang Quanzhen1、Wen Huan Fei1、Naitoh Yoshitaka1、Li Yan Jun1、Sugawara Yasuhiro1 (1.Osaka Univ.)

キーワード:Dipole moment, TiO2

Rutile titanium dioxide (TiO2) has been widely employed as a prototype to investigate the physical and electronic properties of metal oxides. Rutile TiO2(110) surface, with stable single-crystal facet and atomic species point defects including oxygen vacancies and hydroxyl groups, has widespread applicability in the CO oxidation reaction [1]. Recently, the surface potential of rutile TiO2(110) surface, induced by the chemical interaction and surface dipole moment between the tip apex and surface atoms, has been measured [2], in which the latter one strongly affect the potential barrier height [3]. However, the percentage of the dipole moment induced surface potential in the total surface potential has not been investigated yet, which plays an important role in the catalytic mechanism of oxidation reaction.
In this work, by means of Kelvin Probe Force Microscopy (KPFM), we qualitatively measured the dipole moment distribution of rutile TiO2(110) facet and investigated the percentage of the dipole moment induced surface potential in the total surface potential. Experiments were carried out under ultrahigh vacuum (UHV) condition performed at a low temperature of 77 K. And the rutile TiO2(110) surface was cleaned by the cycles of Ar ion bombardment and subsequent annealing at 1000K. Commercial Ir-coated Si cantilever was used after being cleaned with annealing and Ar-ion sputtering. The DC bias voltage added with an ac bias voltage was applied between the tip and the sample. Three lock-in amplifiers were used to detect frequency shift at , and . The contact potential difference (CPD) was numerically calculated from the divided result of and signals and the surface potential induced by dipole moment was obtained from the DC bias feedback.