• Chinese Journal of Chemical Physics
  • Vol. 33, Issue 5, 532 (2020)
Liang Zhang1、2, Junjun Tan1、2, Quanbing Pei1、2, and Shuji Ye1、2、*
Author Affiliations
  • 1Hefei National Laboratory for Physical Sciences at the Microscale, and Department of Chemical Physics, University of Science and Technology of China, Hefei 230026, China
  • 2Synergetic Innovation Center of Quantum Information & Quantum Physics, University of Science and Technology of China, Hefei 230026, China
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    DOI: 10.1063/1674-0068/cjcp2006113 Cite this Article
    Liang Zhang, Junjun Tan, Quanbing Pei, Shuji Ye. Film Thickness and Surface Plasmon Tune the Contribution of SFG Signals from Buried Interface and Air Surface[J]. Chinese Journal of Chemical Physics, 2020, 33(5): 532 Copy Citation Text show less
    A schematic of the near-total-internal-reflection geometry.
    Fig. 1. A schematic of the near-total-internal-reflection geometry.
    The SFG spectra of the carbonyl groups of CaF2 substrate-supported PMMA films prepared with different concentration (0.1 wt%, 0.25 wt%, 0.5 wt%, 1.0 wt%, and 2.0 wt%). (a) ssp and (b) ppp.
    Fig. 2. The SFG spectra of the carbonyl groups of CaF2 substrate-supported PMMA films prepared with different concentration (0.1 wt%, 0.25 wt%, 0.5 wt%, 1.0 wt%, and 2.0 wt%). (a) ssp and (b) ppp.
    The SFG spectra in the C-H stretching region of CaF2 substrate-supported PMMA films prepared with different concentrations (0.1 wt%, 0.25 wt%, 0.5 wt%, 1.0 wt%, and 2.0 wt%). (a) ssp and (b) ppp.
    Fig. 3. The SFG spectra in the C-H stretching region of CaF2 substrate-supported PMMA films prepared with different concentrations (0.1 wt%, 0.25 wt%, 0.5 wt%, 1.0 wt%, and 2.0 wt%). (a) ssp and (b) ppp.
    The fitting strength ratios of (a) $\chi _{\textrm{Peak1}}^{(2)}/\chi _{\textrm{Peak2}}^{(2)}$ and (b) $\chi _{{\rm{ppp}}}^{(2)}/\chi _{{\rm{ssp}}}^{(2)}$ are plotted against solution concentrations used in film preparation.
    Fig. 4. The fitting strength ratios of (a) $\chi _{\textrm{Peak1}}^{(2)}/\chi _{\textrm{Peak2}}^{(2)}$ and (b) $\chi _{{\rm{ppp}}}^{(2)}/\chi _{{\rm{ssp}}}^{(2)}$ are plotted against solution concentrations used in film preparation.
    (a) The relation between the \begin{document}$ \chi _{{\rm{ppp}}}^{(2)}/\chi _{{\rm{ssp}}}^{(2)} $\end{document} ratio and tilt angle \begin{document}$ \theta_{ \rm{C} = \rm{O}} $\end{document} for C = O bond at buried interface (top panel) and air surface (bottom panel). (b) The deduced tilt angle of C = O bond at buried interface (top panel) and air surface (bottom panel).
    Fig. 5. (a) The relation between the \begin{document}$ \chi _{{\rm{ppp}}}^{(2)}/\chi _{{\rm{ssp}}}^{(2)} $\end{document} ratio and tilt angle \begin{document}$ \theta_{ \rm{C} = \rm{O}} $\end{document} for C = O bond at buried interface (top panel) and air surface (bottom panel). (b) The deduced tilt angle of C = O bond at buried interface (top panel) and air surface (bottom panel).
    The SFG spectra of the carbonyl groups of CaF2-Au nanorod-supported PMMA films prepared with different concentration (0.1 wt%, 0.25 wt%, 0.5 wt%, 1.0 wt%, and 2.0 wt%). (a) ssp and (b) ppp.
    Fig. 6. The SFG spectra of the carbonyl groups of CaF2-Au nanorod-supported PMMA films prepared with different concentration (0.1 wt%, 0.25 wt%, 0.5 wt%, 1.0 wt%, and 2.0 wt%). (a) ssp and (b) ppp.
    The fitting strength ratio of $\chi _{\textrm{Peak1}}^{(2)}/\chi _{\textrm{Peak2}}^{(2)}$ is plotted against solution concentrations used in film preparation. The solid circle represents Au-PMMA films and the empty circle represents the pure PMMA films.
    Fig. 7. The fitting strength ratio of $\chi _{\textrm{Peak1}}^{(2)}/\chi _{\textrm{Peak2}}^{(2)}$ is plotted against solution concentrations used in film preparation. The solid circle represents Au-PMMA films and the empty circle represents the pure PMMA films.
    Liang Zhang, Junjun Tan, Quanbing Pei, Shuji Ye. Film Thickness and Surface Plasmon Tune the Contribution of SFG Signals from Buried Interface and Air Surface[J]. Chinese Journal of Chemical Physics, 2020, 33(5): 532
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