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Order enables efficient electron-hole separation at an organic heterojunction with a small energy loss
Donor–acceptor organic solar cells often show low open-circuit voltages (V (OC)) relative to their optical energy gap (E (g)) that limit power conversion efficiencies to ~12%. This energy loss is partly attributed to the offset between E (g) and that of intermolecular charge transfer (CT) states at...
Autores principales: | , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2018
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5773693/ https://www.ncbi.nlm.nih.gov/pubmed/29348491 http://dx.doi.org/10.1038/s41467-017-02457-5 |
Sumario: | Donor–acceptor organic solar cells often show low open-circuit voltages (V (OC)) relative to their optical energy gap (E (g)) that limit power conversion efficiencies to ~12%. This energy loss is partly attributed to the offset between E (g) and that of intermolecular charge transfer (CT) states at the donor–acceptor interface. Here we study charge generation occurring in PIPCP:PC(61)BM, a system with a very low driving energy for initial charge separation (E (g)−E (CT) ~ 50 meV) and a high internal quantum efficiency (η (IQE) ~ 80%). We track the strength of the electric field generated between the separating electron-hole pair by following the transient electroabsorption optical response, and find that while localised CT states are formed rapidly (<100 fs) after photoexcitation, free charges are not generated until 5 ps after photogeneration. In PIPCP:PC(61)BM, electronic disorder is low (Urbach energy <27 meV) and we consider that free charge separation is able to outcompete trap-assisted non-radiative recombination of the CT state. |
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