1995
DOI: 10.1021/j100039a029
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Langmuir Film-Forming and Second Harmonic Generation Properties of Lanthanide Complexes

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Cited by 60 publications
(29 citation statements)
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“…10 In the present study, the wavelength of the second harmonic (650 nm) is further away from the wavelength of maximum absorption in solution (493 nm), leading to a much smaller enhancement factor. To be able to compare the hyperpolarizability values obtained at different fundamental wavelengths λ fund , the static hyperpolarizability 0 , corrected for the resonance enhancement, can be calculated on the basis of the wavelength of maximum absorption λ max for the noncentrosymmetric chargetransfer band and the two-level model: 22 With this correction factor and the wavelength of maximum absorption λ max from the spectra shown in Figure 3, we arrive at 0 values for our BMPP complexes of (31 ( 1) × 10 -30 esu, while the previously obtained value for the 4-[4-(dimethylamino)styryl]-1-hexadecylpyridinium iodide from LB films 9 results in a 0 value ranging from 30 × 10 -30 to 45 × 10 -30 esu. It is clear, then, that the larger hyperpolarizability values for the complexes with lanthanide counteranions calculated from the film susceptibility are overestimated, due to the positive influence of the better film-forming properties for the latter complexes.…”
Section: Resultsmentioning
confidence: 60%
“…10 In the present study, the wavelength of the second harmonic (650 nm) is further away from the wavelength of maximum absorption in solution (493 nm), leading to a much smaller enhancement factor. To be able to compare the hyperpolarizability values obtained at different fundamental wavelengths λ fund , the static hyperpolarizability 0 , corrected for the resonance enhancement, can be calculated on the basis of the wavelength of maximum absorption λ max for the noncentrosymmetric chargetransfer band and the two-level model: 22 With this correction factor and the wavelength of maximum absorption λ max from the spectra shown in Figure 3, we arrive at 0 values for our BMPP complexes of (31 ( 1) × 10 -30 esu, while the previously obtained value for the 4-[4-(dimethylamino)styryl]-1-hexadecylpyridinium iodide from LB films 9 results in a 0 value ranging from 30 × 10 -30 to 45 × 10 -30 esu. It is clear, then, that the larger hyperpolarizability values for the complexes with lanthanide counteranions calculated from the film susceptibility are overestimated, due to the positive influence of the better film-forming properties for the latter complexes.…”
Section: Resultsmentioning
confidence: 60%
“…The secondharmonic generation (SHG) experiment shows that there is a tilt angle of 44°of the chromophores, relative to the normal of the substrate, 10 which is similar to that obtained from films of the hemicyanine halides. 9,11 The electronic absorption spectra of the P 3 n LB film is shown in Figure 2a. The λ max occurs at ca.…”
Section: Characterization Of Lb Film and Dye-ito Electrodementioning
confidence: 99%
“…The inset Fig. 4 shows a plotter absorbance at 294 nm against number of layers deposited, the linear dependence of the absorbance on the number of layers can be obtained for 11, 21 and 31 layers LB films; considering that the intensity of absorption is determined by the amount of the complex a deviation from linearity was observed just for one layer LB deposited, it could be explained by the sensitivity of UV-vis measurements [16,17]. Fig.…”
Section: Monolayer Behaviors and Lb Film Fabricationmentioning
confidence: 94%