• Chinese Journal of Chemical Physics
  • Vol. 33, Issue 5, 554 (2020)
Cai-he Liu1,2, Rui-peng Bai1,2, Yu Bai1, Yuan Guo1,2, and Zhen Zhang1,2,*
Author Affiliations
  • 1Beijing National Laboratory of Molecular Sciences, State Key Laboratory of Molecular Reaction Dynamics, CAS Research/Education Center for Excellence in Molecular Sciences, Institute of Chemistry, Chinese Academy of Sciences, Beijing 100190, China
  • 2University of the Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.1063/1674-0068/cjcp2007129 Cite this Article
    Cai-he Liu, Rui-peng Bai, Yu Bai, Yuan Guo, Zhen Zhang. Si(111) Electrode/Electrolyte Interfacial Studied by in-situ Second Harmonic Generation[J]. Chinese Journal of Chemical Physics, 2020, 33(5): 554 Copy Citation Text show less
    Air/Si(111) interface rotation diagram
    Fig. 1. Air/Si(111) interface rotation diagram
    (a) SHG response curve of air/Si(111) interface with the pp polarization combination. The circles in the figure represent experimental data points and the solid line represents the fitted curves. (b) Polar map of the air/Si(111) interface. The red circle represents the intensity of the SHG signal and the polar axis represents the angle
    Fig. 2. (a) SHG response curve of air/Si(111) interface with the pp polarization combination. The circles in the figure represent experimental data points and the solid line represents the fitted curves. (b) Polar map of the air/Si(111) interface. The red circle represents the intensity of the SHG signal and the polar axis represents the angle
    (a) Cyclic voltammogram (CV) curve measured from the Si(111)/CH\begin{document}$ _3 $\end{document}CN system with a scan rate of 50 mV/s. (b) The Mott-Schottky diagram from the Si(111)/CH\begin{document}$ _3 $\end{document}CN system measured at 1500 Hz. The red dots are the experimental data, and the red solid line is obtained by fitting using Eq.(5). The experiment temperature was 298 K
    Fig. 3. (a) Cyclic voltammogram (CV) curve measured from the Si(111)/CHUnknown environment 'document'CN system with a scan rate of 50 mV/s. (b) The Mott-Schottky diagram from the Si(111)/CHUnknown environment 'document'CN system measured at 1500 Hz. The red dots are the experimental data, and the red solid line is obtained by fitting using Eq.(5). The experiment temperature was 298 K
    The potential-dependent SHG intensity of the Si(111)/CH\begin{document}$ _3 $\end{document}CN system at azimuthal angles \begin{document}$ \phi $\end{document} = 0\begin{document}$ ^{\circ} $\end{document}, 30\begin{document}$ ^{\circ} $\end{document} and 60\begin{document}$ ^{\circ} $\end{document}. The red dots are the experimental data, and the black solid line is the fitting curve.
    Fig. 4. The potential-dependent SHG intensity of the Si(111)/CHUnknown environment 'document'CN system at azimuthal angles Unknown environment 'document' = 0Unknown environment 'document', 30Unknown environment 'document' and 60Unknown environment 'document'. The red dots are the experimental data, and the black solid line is the fitting curve.
    Table 1. Fitting results of potential dependent SHG response for different polarization combinations at $ \phi $=30$ ^{\circ} $
    Table 2. Fitting results of potential dependent SHG response for different polarization combinations at $\phi$=0$^{\circ}$. The relative phase $\theta$ cannot be obtained by Eq.(6), and the values are not shown in the table.
    Table 3. Fitting results of potential dependent SHG response for different polarization combinations at $ \phi $=60$ ^{\circ} $
    Cai-he Liu, Rui-peng Bai, Yu Bai, Yuan Guo, Zhen Zhang. Si(111) Electrode/Electrolyte Interfacial Studied by in-situ Second Harmonic Generation[J]. Chinese Journal of Chemical Physics, 2020, 33(5): 554
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