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Energy of the hot charge carriers excited by longer wavelength photons is below trap-related states.
This process prevailed over plasmonic photogeneration of the hot charge carriers at lower excitation wavelengths, while energy of the hot charge carrier's photoexcited by longer wavelength photons was lower than the energy of the trap states.
Only in the case of the samples excited by 627 and 736 nm, the negative absorption signal, e.g., generation of the hot charge carriers can be seen.
It should be mentioned that in numerous studies, hot charge carrier generation or photovoltaic quantum efficiency spectra correlate with the absorption spectra of the plasmonic absorber.
We also provide theoretical modelling of the electron generation mechanisms and for the first time calculate the contribution of hot charge carriers.
It seems that at lower excitation, wavelength influence of the DLC matrix results in suppression of the surface plasmon resonance-related hot charge carrier photogeneration.
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Jailaubekov, A. E. et al. Hot charge-transfer excitons set the time limit for charge separation at donor/acceptor interfaces in organic photovoltaics.
Firstly, we used quantum-chemical calculations to illustrate exciton-dissociation and charge-recombination processes at the DTDCTB/C60 interface and particularly emphasized the major role of hot charge-transfer states in the exciton-dissociation processes.
There, the hot charged particles cause problems wherever they go.
However, for certain grades of steel, the hot charging process may affect the steel surface quality.
Hot charging of continuous cast steel billets is usually considered an effective method for recovering heat.
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