Rapid exciton diffusion in next generation organic semiconductors and its implications for charge photogeneration
Justin M. Hodgkiss b
a MacDiarmid Institute for Advanced Materials and Nanotechnology, New Zealand., PO Box 600, Wellington, New Zealand
b School of Chemical and Physical Sciences,Victoria University of Wellington, New Zealand, New Zealand
Materials for Sustainable Development Conference (MATSUS)
Proceedings of nanoGe Spring Meeting 2022 (NSM22)
#OrgCD22. Charge Dynamics of State-of-the-art Organic Solar Cells
Online, Spain, 2022 March 7th - 11th
Organizers: Ardalan Armin and Safa Shoaee
Invited Speaker, Justin M. Hodgkiss, presentation 244
DOI: https://doi.org/10.29363/nanoge.nsm.2022.244
Publication date: 7th February 2022

Modest exciton diffusion lengths dictate the need for nanostructured bulk heterojunctions in organic photovoltaic (OPV) cells, however, this morphology compromises charge collection. Here, we reveal rapid exciton diffusion in films of a fused-ring electron acceptor that, when blended with a donor, already outperforms fullerene-based OPV cells. Temperature-dependent ultrafast exciton annihilation measurements are used to resolve a quasi-activationless exciton diffusion coefficient of at least 2 ×10-2 cm2 / s – substantially exceeding typical organic semiconductors, and consistent with the 20-50 nm domain sizes in optimized blends.[1] Enhanced 3-dimensional diffusion accounted for computationally [2] and is shown to arise from molecular and packing factors; the rigid planar molecular structure is associated with low reorganization energy, good transition dipole moment alignment, high chromophore density, and low disorder – all enhancing long-range resonant energy transfer. Relieving exciton diffusion constraints has important implications for OPVs; large, ordered, and pure domains enhance charge separation and transport, and suppress recombination, thereby boosting fill factors. Further enhancements to diffusion lengths may even obviate the need for the bulk heterojunction morphology [3].

 

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