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Beilstein J. Nanotechnol. 2015, 6, 2252–2262, doi:10.3762/bjnano.6.231
Figure 1: SEM images of In2O3 mesoporous films (a,d), ZnO platelet crystallites (b,e) and anodic TiO2 nanotub...
Figure 2: Spectral dependence of IPCE for ZnO/CdS (a), TiO2/CdS (b), and In2O3/CdS heterostructures (c). IPCE...
Figure 3: CdS band gap Eg dependence on the number of SILAR deposition cycles.
Figure 4: Spectral dependence of IPCE in lnY–hν coordinates for ZnO/CdS (a), TiO2/CdS (b), and In2O3/CdS hete...
Figure 5: Raman spectra for TiO2/CdS (a,b), ZnO/CdS (c,d), and In2O3/CdS (e,f) films. Excitation: 473 nm/25 μ...
Figure 6: Approximation of Raman spectrum for TiO2/CdS film (N = 30) in the vicinity of the CdS LO band by su...
Figure 7: Intensity of CdS LO band as a function of the SILAR cycle number. Excitation: 473 nm/25 μW (a) and ...
Figure 8: Position of CdS LO band as a function of the SILAR cycle number. Excitation: 473 nm/25 μW (a) and 5...
Figure 9: FWHM of CdS LO band as a function of the SILAR cycle number. Excitation: 473 nm/25 μW (a) and 532 n...
Figure 10: Intensity ratio of CdS 2LO and LO bands as a function of the SILAR cycle number. Excitation: 473 nm...
Figure 11: Intensity ratio of CdS SO and LO bands as a function of the SILAR cycle number. Excitation: 473 nm/...