23. The excess oxygen and the decomposed In may react to form In2O3. The analyzed oxygen content is enough just to form stoichiometric TiO2 with an estimated concentration of 76 at.% and In2O3 with 8 at.%. An HRTEM image of the composite film is presented in Figure 7a. The slightly dark sphere-like nanocrystals are clearly dispersed, with a size of approximately 15 nm. The selected area Selleckchem SHP099 (dotted

line) is enlarged in Figure 7b for easier viewing. Fast Momelotinib solubility dmso Fourier transform (FFT) analysis of the region (circle in Figure 7b) reveals the details of the local structure in the nanocrystal. Figure 7c presents the corresponding FFT diffraction pattern, which can be indexed to cubic InSb. The spots labeled A, B, and C correspond to crystal faces of (110), (1-10), and (200) in the Fedratinib cubic InSb, with plane widths of 0.452, 0.466, and 0.330 nm, respectively. The angles labeled A-X-B, A-X-C, and B-X-C are 89°, 46°,

and 43°. The standard data (JCPDS 6–208) indicates a plane width of 0.458 nm at both (110) and (1-10), and 0.324 nm at (200), with an angle of 90° for A-X-B and 45° for both A-X-C and B-X-C. The analysis results are close to the standard data. The observed grain is thus found to be cubic InSb nanocrystal. Therefore, InSb-added TiO2 nanocomposite film produces a composite with InSb nanocrystals dispersed in a multiphase matrix composing TiO2 and In2O3. The mean grain size of the InSb nanocrystals is estimated to be 18 nm using Scherrer’s formula [22] in XRD peak fitting. This size is nearly the same as that of the observed InSb nanocrystals. This is small enough to exhibit the quantum size effects because of the exciton Bohr radius of 65.5 nm in InSb [14]. Furthermore, the ground state transition of electron–hole pairs in the semiconductor nanocrystal is calculated by the following formula [23, 24]: E = E g + (ħπ)2/2μR 2 − 1.8e 2/4π ∈ ∈ 0 R, where E g is the bulk band gap, ħ is the reduced Planck constant, μ is the reduced mass of an electron–hole pair, R is the effective Bohr radius, e is the electron charge, and

∈ is the background dielectric constant of InSb. GPX6 Hence, the ground state transition of the InSb nanocrystals is calculated to be 0.78 eV, which corresponds well to the onset absorption containing 18 at.% (In and Sb) (Figure 6). Therefore, the optical absorption shift is obviously due to quantum size effects of the InSb nanocrystals embedded in the multiphase matrix, TiO2 and In2O3. Figure 6 Typical optical absorption spectra of InSb-added TiO 2 composite film. With a phase mixture of InSb, TiO2, and In2O3, containing 18 at.% (In + Sb). Figure 7 Direct observation of InSb-added TiO 2 nanocomposite film. With a phase mixture of InSb, TiO2, and In2O3, containing 18 at.% (In + Sb). (a) HRTEM image. (b) Enlarged image for easier viewing. (c) FFT diffraction pattern of the selected area, indicated by the circle in (b).