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84879837410
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Absorption spectra and differential absorption spectra upon photoexcitation were recorded after depositing the films on quartz Quasi reference electrode: Ag wire. Supporting electrolyte: tetrabutylammonium hexafluorophosphate 0.1 M in acetonitrile
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Absorption spectra and differential absorption spectra upon photoexcitation were recorded after depositing the films on quartz. Differential absorption spectra upon spectroelectrochemical oxidation were recorded after depositing the films on ITO. CE: Pt wire. Quasi reference electrode: Ag wire. Supporting electrolyte: tetrabutylammonium hexafluorophosphate 0.1 M in acetonitrile.
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Differential Absorption Spectra Upon Spectroelectrochemical Oxidation Were Recorded after Depositing the Films on ITO. CE: Pt Wire
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18
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84879839571
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Please note that the signal ranging from 720 to 800 nm is affected by an artifact due to overlap between pump and probe wavelengths and was consequently omitted from the plots
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Please note that the signal ranging from 720 to 800 nm is affected by an artifact due to overlap between pump and probe wavelengths and was consequently omitted from the plots.
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19
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84879837155
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-2), the P3HT:PCBM 1:1 reference sample showed the same pronounced features as upon excitation with a wavelength of 550 nm with the same intensity. The reason for such a behavior is not unambiguously identified at this stage. A likely rationale implies direct generation of CT states even though the sample was excited with energy smaller than the bandgap of P3HT. Residual contributions from the seed laser can cause erroneous excitation of P3HT. In the experiments presented in this communication, direct charge generation in P3HT in the P3HT:PCPDTBT:PCBM 0.9:0.1:1 films are excluded because P3HT:PCBM 1:1 films showed no significant features under the same experimental conditions
-
-2), the P3HT:PCBM 1:1 reference sample showed the same pronounced features as upon excitation with a wavelength of 550 nm with the same intensity. The reason for such a behavior is not unambiguously identified at this stage. A likely rationale implies direct generation of CT states even though the sample was excited with energy smaller than the bandgap of P3HT. Residual contributions from the seed laser can cause erroneous excitation of P3HT. In the experiments presented in this communication, direct charge generation in P3HT in the P3HT:PCPDTBT:PCBM 0.9:0.1:1 films are excluded because P3HT:PCBM 1:1 films showed no significant features under the same experimental conditions.
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22
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84879837512
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n are the amplitudes of the transients. Nevertheless, only absorption time profiles at 565 and 650 nm were shown in Figure 2 since they directly relate to the investigated hole transfer process
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n are the amplitudes of the transients. Nevertheless, only absorption time profiles at 565 and 650 nm were shown in Figure 2 since they directly relate to the investigated hole transfer process.
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23
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77950292422
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M. Morana, H. Azimi, G. Dennler, H. J. Egelhaaf, M. Scharber, K. Forberich, J. Hauch, R. Gaudiana, D. Waller, Z. Zhu, K. Hingerl, S. S. v. Bavel, J. Loos, C. J. Brabec, Adv. Funct. Mater. 2010, 20, 1180.
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Loos, J.13
Brabec, C.J.14
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