Excitonic Processes in Condensed Matter 2001
DOI: 10.1142/9789812811387_0072
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OPTICAL SECOND HARMONIC SPECTROSCOPY OF THE ANATASE TiO2 (101) FACE

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Cited by 2 publications
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“…For this reason, SHG is sensitive to the surfaces or interfaces of materials with centrosymmetric bulk structures. It has already been applied to the analyses of electronic states on the surfaces and interfaces [7][8][9][10][11][12][13][14]. Maeda et al succeeded in measuring SHG from steps on the Au (887) and (443) single crystal surfaces [9].…”
Section: Introductionmentioning
confidence: 99%
“…For this reason, SHG is sensitive to the surfaces or interfaces of materials with centrosymmetric bulk structures. It has already been applied to the analyses of electronic states on the surfaces and interfaces [7][8][9][10][11][12][13][14]. Maeda et al succeeded in measuring SHG from steps on the Au (887) and (443) single crystal surfaces [9].…”
Section: Introductionmentioning
confidence: 99%
“…Note that the spectra shown in Fig. 1 are similar to those of anatase TiO 2 (101) 20. The energy difference between the band gap and the lowest SH peak is 0.7 eV for the anatase TiO 2 (101), while that for the rutile TiO 2 (15 15 4) surface is about 0.6 eV.…”
Section: Resultsmentioning
confidence: 59%
“…In our previous work,21 we succeeded in detecting the signals of the steps periodically aligned on the TiO 2 surfaces selectively by means of second harmonic generation (SHG)13–20 with nearly normal incident fundamental excitation. We found that both high index TiO 2 (15 15 4) and (671) surfaces with steps have large nonlinear susceptibility elements $\chi_{xxx}^{(2)}$ and $\chi_{xyy}^{(2)}$ , with x representing the [0 0 1] and y representing the [1 1 0] directions.…”
Section: Introductionmentioning
confidence: 99%