2020
DOI: 10.1039/d0tc01077d
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Kinetic model for photoluminescence quenching by selective excitation of D/A blends: implications for charge separation in fullerene and non-fullerene organic solar cells

Abstract:

Our findings demonstrate the importance of kinetic factors in determining the overall charge separation efficiency in D/A systems.

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Cited by 19 publications
(30 citation statements)
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“…[84][85][86][87] Organic donor:acceptor blends show strongly quenched emission relative to neat materials, attributed to exciton dissociation and subsequent nonradiative charge recombination at the donor/acceptor interface; this PL quenching is widely used as an assay of efficient exciton separation in organic blends. [88][89][90][91] By contrast, in neat perovskite films, PL emission comes from the radiative recombination of free charge carriers, with the main competing pathway being charge localization into nonradiative trap states. [41,92] Such nonradiative charge trapping is most dominant at low light fluxes, but becomes at least partially suppressed at high light intensities (e.g., 1 sun), attributed to trap filling.…”
Section: Materials Absorbance and Photoluminescencementioning
confidence: 99%
“…[84][85][86][87] Organic donor:acceptor blends show strongly quenched emission relative to neat materials, attributed to exciton dissociation and subsequent nonradiative charge recombination at the donor/acceptor interface; this PL quenching is widely used as an assay of efficient exciton separation in organic blends. [88][89][90][91] By contrast, in neat perovskite films, PL emission comes from the radiative recombination of free charge carriers, with the main competing pathway being charge localization into nonradiative trap states. [41,92] Such nonradiative charge trapping is most dominant at low light fluxes, but becomes at least partially suppressed at high light intensities (e.g., 1 sun), attributed to trap filling.…”
Section: Materials Absorbance and Photoluminescencementioning
confidence: 99%
“…Those findings motivated us to extend the previous model in ref to include the influence of the electric field on the kinetics of charge separation at the D/A interface. We also refined the model by considering the effects of energetic, positional, and electronic coupling disorders on those processes.…”
Section: Introductionmentioning
confidence: 64%
“…Note from eq that if the donor is not efficient to dissociate the excitons, then [ S 1,A ′] ≈ [ S 1,A ] and Q A ≈ 0. The solution of the model’s differential equations in steady-state approximation gives the quenching efficiency for the acceptor and the donor excitations (further details can be found in ref ): and where the k ’s in eqs and are the rates that characterizes all possible electronic transitions after the formation of the singlet state either in the acceptor (eq ) or in the donor (eq ). In Table , we detail all those rates in eqs and with the corresponding electronic transitions and the frontier molecular orbitals involved (HOMO, highest occupied molecular orbital, and LUMO, lowest unoccupied molecular orbitals).…”
Section: Methodsmentioning
confidence: 99%
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