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TiO2 B

Wang, Q., Wen, Z., Li, J., 2006. A hybrid supercapacitor fabricated with a carbon nanotube cathode and a Tio2—B nanowite anode. Advanced Functional Materials 16, 2141—2146. [Pg.399]

Fig. 2. UV-VISdiffiise reflectance sp>ectra of (a) TiO2-400°C, (b) CdS-IPA-800 C, (c) CdS-Ti02, (d) CdS-Ti02 physically mixed (PM). Fig. 2. UV-VISdiffiise reflectance sp>ectra of (a) TiO2-400°C, (b) CdS-IPA-800 C, (c) CdS-Ti02, (d) CdS-Ti02 physically mixed (PM).
Figure 6.6 Vibrational coherence on a pNB-adsorbed TiO2(110) surface, (a) The raw SH intensity, (b) the modulated component, (c) the Fourier-transformed spectrum, the gray lines show the transformed spectrum. The spectrum simulated with Lorentzian functions is overlaid with broken lines. The pNB-adsorbed surface was irradiated in air with p-polarized pump (8mjcm ) and p-polarized probe (8mjcm ) pulses of a 550-nm wavelength. Figure 6.6 Vibrational coherence on a pNB-adsorbed TiO2(110) surface, (a) The raw SH intensity, (b) the modulated component, (c) the Fourier-transformed spectrum, the gray lines show the transformed spectrum. The spectrum simulated with Lorentzian functions is overlaid with broken lines. The pNB-adsorbed surface was irradiated in air with p-polarized pump (8mjcm ) and p-polarized probe (8mjcm ) pulses of a 550-nm wavelength.
White, J. M., Szanyi, J. and Henderson, M. A. (2003) The photon-driven hydrophilicity of titania A model study using TiO2(110) and adsorbed trimethyl acetate./. Phys. Chem. B, 107, 9029—9033. [Pg.116]

Ishibashi, T, Uetsuka, H. and Onishi, H. (2004) An ordered retinoate monolayer prepared on rutile TiO2(110)./. Phys. Chem. B, 108, 17166-17170. [Pg.116]

Molina LM, Rasmussen MD, Hammer B. 2004. Adsorption of O2 and oxidation of CO at Au nanoparticles supported by TiO2(110). J Chem Phys 120 7673-7680. [Pg.591]

Oekermann, T. Zhang, D. Yoshida, T. Minoura, H., Electron transport and back reaction in nanocrystalline Tio2 films prepared by hydrothermal crystallization. J. Phys. Chem. B 2004, 108, 2227-2235. [Pg.472]

Figure 5 Temperature-programmed desorption/oxidation for (a) ethanol and (b) acetaldehyde on TiO2. (From Ref. 48.)... Figure 5 Temperature-programmed desorption/oxidation for (a) ethanol and (b) acetaldehyde on TiO2. (From Ref. 48.)...
Figure 5 Shifts in the absorption spectra of various types of TiO2 photocatalysts (shown in Table 1) implanted with the same amounts of V ions, (a) original unimplanted pure P-25, (b) V/F-6, (c) V/F-4, (d) V/P-25, (e) V/F-2, (f) V/F-1. Amount of V ion implanted was 6.6 X 10 mol/g (3.4 x 10 wl%). Figure 5 Shifts in the absorption spectra of various types of TiO2 photocatalysts (shown in Table 1) implanted with the same amounts of V ions, (a) original unimplanted pure P-25, (b) V/F-6, (c) V/F-4, (d) V/P-25, (e) V/F-2, (f) V/F-1. Amount of V ion implanted was 6.6 X 10 mol/g (3.4 x 10 wl%).
Figure 6 UV-vis absorption spectra (diffuse reflectance) of the original undoped pure TiO2 (a) and TiO, chemically doped with Cr ions (b -e ). Cr ions chemically doped in 10" mol/g (a) undoped original pure TiOi (P-25), (b ) 16, (c ) 200, (d i 1000, (e ) 2000. The TiO2 photocatalysts chemically doped with Cr ions did not exhibit any photocatalytic reactivity. Figure 6 UV-vis absorption spectra (diffuse reflectance) of the original undoped pure TiO2 (a) and TiO, chemically doped with Cr ions (b -e ). Cr ions chemically doped in 10" mol/g (a) undoped original pure TiOi (P-25), (b ) 16, (c ) 200, (d i 1000, (e ) 2000. The TiO2 photocatalysts chemically doped with Cr ions did not exhibit any photocatalytic reactivity.
Figure 9 Effect of the Cr- and V-ion-implantation on the photocatalytic reactivity of TiO2 under outdoor solar beam irradiation for the photocatalytic reaction of CH3CCH with H2O leading a hydogenolysis reaction of CH3CCH with H2O at 295 K. A fine, B cloudy weather (solar intensity during fine weather 12 inW/cm amount of photocatalyst 6.0 g). Figure 9 Effect of the Cr- and V-ion-implantation on the photocatalytic reactivity of TiO2 under outdoor solar beam irradiation for the photocatalytic reaction of CH3CCH with H2O leading a hydogenolysis reaction of CH3CCH with H2O at 295 K. A fine, B cloudy weather (solar intensity during fine weather 12 inW/cm amount of photocatalyst 6.0 g).
Figure 12 XANES (left) and ET-EXAES spectra (right) of Cr-ion chemically doped TiO2 (a, A) and Cr-ion-implanted TiOi catalysts (b, B). Figure 12 XANES (left) and ET-EXAES spectra (right) of Cr-ion chemically doped TiO2 (a, A) and Cr-ion-implanted TiOi catalysts (b, B).
Fig. 2.11 Structure in the vicinity of the shear plane for the shear operation (/ifcZ) [011] of a TiOj-type structure, (a) (121)5[0il] (b) (132) [0il] (c) (011)2[0il] the structure obtained after only operation (3) on TiO2 without the elimination of an oxygen-only plane. The structure is called an APB (anti phase boundary) or twin structure, and is similar to the shear structure of (110)j[li0] of ReOj (see Fig. 2.6(a)). Note the atomic arrangement in the zones framed by dotted lines (see also Fig. 2.113). Fig. 2.11 Structure in the vicinity of the shear plane for the shear operation (/ifcZ) [011] of a TiOj-type structure, (a) (121)5[0il] (b) (132) [0il] (c) (011)2[0il] the structure obtained after only operation (3) on TiO2 without the elimination of an oxygen-only plane. The structure is called an APB (anti phase boundary) or twin structure, and is similar to the shear structure of (110)j[li0] of ReOj (see Fig. 2.6(a)). Note the atomic arrangement in the zones framed by dotted lines (see also Fig. 2.113).
Fig. 8.20. (a) Densities of states of the surface clusters (Ti40,5) (solid line) and (Ti40i6)" (dashed line) calculated by the DV-Za method, (b) Densities of states of the clusters (Ti30,4) (solid line) and (TijO,) - (dashed line) representative of solid bulk TiOj calculated by the DV-Za method, (c) Ultraviolet photoelectron spectra for the ordered (dashed line) and bombarded (solid line) (110) surface of rutile (TIO2) (after Tsukada et al., 1983 reproduced with the publisher s permission). [Pg.411]

Chandrasekharan N. and Kamat, P. V. (2000). Improving the photoelectrochemical performance of nanostructured tio2 films by adsorption of gold nanoparticles. J. Phys. Chem. B, 104 10851-10857. [Pg.571]

Fig. 12. (a) Formate O Is XPD pattern obtained from TiO2(H0)2xl-[HCOO] , and (b) a sketch of the local adsorption geometry [84-86],... [Pg.221]

Fig. 10. FT-RAIRS spectrum of rhodium dicarbonyl Rh(CO)2 on TiO2(H0) [56, 69, 70] following dissociative adsorption of Rh2C04Cl2 (a). The molecule is reformed after desorption of the CO at 450K following exposure to lOOL of CO (b). Reaction of Rh(CO)2 with hydrogen forms the monocarbonyl Rh(H)CO [71]. Fig. 10. FT-RAIRS spectrum of rhodium dicarbonyl Rh(CO)2 on TiO2(H0) [56, 69, 70] following dissociative adsorption of Rh2C04Cl2 (a). The molecule is reformed after desorption of the CO at 450K following exposure to lOOL of CO (b). Reaction of Rh(CO)2 with hydrogen forms the monocarbonyl Rh(H)CO [71].
One may have expected that the transmission band should remain invariant with (j), since P couples to Vsym(OCO) of both species equally at all ( ). In fact the doublet structure in the transmission band was ascribed to the presence of the two formate species. However, while species A has C2V symmetry, the symmetry of formate species B is lower because of the incorporation of one of the formate oxygen atoms in the TiO2(110) top rows (Figl4). The result is that Vsym(OCO) for B also has a component parallel to the surface which can couple to Pt, resulting in an absorption band. This coupling is possible at (j>= 90°, but not at ( )= 0°, resulting (because of its coincident energy) in the apparent (j) dependence in the Vsym(OCO) transmission band. [Pg.539]

Bennett RA, Pang CL, Perkins N, Smith RD, Morrall P, Kvon RI, Bowker M (2002) Surface structures in the SMSI state Pd on (1x2) reconstructed TiO2(110). J Phys Chem B 106 4688... [Pg.172]

Figure 21 ALISS polar scans of a TiO2(110)-p(l x 1) surface taken along the (a) [001] direction and (b) [—110] direction using 1-keV Li" " ions backscattered at 160°. The solid circles are experimental data points and the solid curve is the result of theoretical calculations. Dotted lines demonstrate simulations for an error in critical angle by +1.0°. The dashed line shows the simulations for the bulk structure shown in Figure 20. (From Ref. 41.)... Figure 21 ALISS polar scans of a TiO2(110)-p(l x 1) surface taken along the (a) [001] direction and (b) [—110] direction using 1-keV Li" " ions backscattered at 160°. The solid circles are experimental data points and the solid curve is the result of theoretical calculations. Dotted lines demonstrate simulations for an error in critical angle by +1.0°. The dashed line shows the simulations for the bulk structure shown in Figure 20. (From Ref. 41.)...
Figure 10 Plots of the Au4f7/2 core-level binding energy as a function of Au cluster coverage (ranging from 0.02 MLE to bulk) on TiO2(110)(A) and Si02(B) surfaces. (From Ref. 160.)... Figure 10 Plots of the Au4f7/2 core-level binding energy as a function of Au cluster coverage (ranging from 0.02 MLE to bulk) on TiO2(110)(A) and Si02(B) surfaces. (From Ref. 160.)...

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