2019
DOI: 10.1007/s10854-019-00721-6
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Energy transfer processes in electrochemical P3HT thin films

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Cited by 6 publications
(6 citation statements)
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“…The value of Eonset can be explained to the P3HT in terms of: (i) the conjugation length of the polymeric chains, the shorter the length of the conjugated polymeric segment, the greater the value of Eonset [21] and (ii) the feature regioregular of the polymeric main chain, that is, Eonset increase if the regioregularity decrease of the polymeric chains [28,29]. The data obtained for Eonset are in accordance with the literature [18,30] and in concordance of Kinoshita et al where the characteristic absorption range for the regioregular P3HT is 415 to 650 nm [29]. The values in Table 1 show Eonset of P3HT decreases in the presence of reduced graphene oxide (RGO).…”
Section: Resultssupporting
confidence: 87%
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“…The value of Eonset can be explained to the P3HT in terms of: (i) the conjugation length of the polymeric chains, the shorter the length of the conjugated polymeric segment, the greater the value of Eonset [21] and (ii) the feature regioregular of the polymeric main chain, that is, Eonset increase if the regioregularity decrease of the polymeric chains [28,29]. The data obtained for Eonset are in accordance with the literature [18,30] and in concordance of Kinoshita et al where the characteristic absorption range for the regioregular P3HT is 415 to 650 nm [29]. The values in Table 1 show Eonset of P3HT decreases in the presence of reduced graphene oxide (RGO).…”
Section: Resultssupporting
confidence: 87%
“…Whereas the energy transfer processes depend on a series of photophysical processes it is, in general, necessary to correlate different experimental techniques to be fully clarified. Specifically, for studies involving energy transfer, the Emission Ellipsometry (EE) [17] using Stokes Parameter Spectroscopy (SPS) [18] is a powerful technique that allows to fully describe the polarization state of the light emitted with the aid of Stokes Theory [19]. Thus, it is possible to apply EE to study energy transfer from photo-excited carriers in polymeric and conjugated materials [18][19][20][21].…”
Section: Introductionmentioning
confidence: 99%
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“…Thus, a redshift occurs when the excitation energy is decreased (longer wavelength); in the case shown, the maximum PL changes from 410 to 510 nm. Furthermore, when excited at 320, 340, and 360 nm, the PL spectra of CDQs a showed similar emission intensities, which may imply similarity in the quantum luminescence efficiency ( Therézio et al, 2011 ; 2013 ) and the same energy transfer rate (Stokes shift) ( Schura et al, 2019 ). However, in the PL spectra of CQDs b , when excited at these same energies (320, 340, and 360 nm), there is a substantial increase in the PL intensity as the excitation changes, certainly implying a higher luminescence quantum efficiency.…”
Section: Resultsmentioning
confidence: 89%
“…Conjugated polymers have found many uses in devices such as thin-film transistors, organic photovoltaics, and organic light-emitting diodes. Their use is driven, in part, by their lower cost and weight when compared to similar inorganic counterparts. The conjugated polymer found in the active layer of such devices exhibits optoelectronic processes such as exciton formation, charge separation, recombination, trapping, and charge transport. There are many structural factors that can affect these properties, and there is significant evidence that a major contributor is the conformation of the conjugated polymers in the active layer. Moreover, there are several factors that affect the polymer conformation in the active layer, such as the concentration of the polymer in predeposition solution, polymer–solvent interactions, and post-processing methods such as annealing at elevated temperatures. …”
Section: Introductionmentioning
confidence: 99%