1. Photocurrent generation in polymer-fullerene bulk heterojunctions
- Author
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Valentin D. Mihailetchi, Jan C. Hummelen, L. J. A. Koster, Paul W. M. Blom, Molecular Energy Materials, Zernike Institute for Advanced Materials, Stratingh Institute of Chemistry, and Photophysics and OptoElectronics
- Subjects
Photocurrent ,PHOTOINDUCED ELECTRON-TRANSFER ,PLASTIC SOLAR-CELLS ,Materials science ,Fullerene ,FIELD-ASSISTED DISSOCIATION ,Condensed matter physics ,Polymer-fullerene bulk heterojunction solar cells ,INSULATORS ,Photoconductivity ,General Physics and Astronomy ,RECOMBINATION ,Heterojunction ,Electron hole ,TRANSIENT ,CHARGE-TRANSFER STATES ,Molecular physics ,Dissociation (chemistry) ,TRANSPORT ,PHOTOGENERATION ,Bound state ,ComputingMethodologies_DOCUMENTANDTEXTPROCESSING ,Physics::Chemical Physics ,GeneralLiterature_REFERENCE(e.g.,dictionaries,encyclopedias,glossaries) ,TEMPERATURE - Abstract
The photocurrent in conjugated polymer-fullerene blends is dominated by the dissociation efficiency of bound electron-hole pairs at the donor-acceptor interface. A model based on Onsager's theory of geminate charge recombination explains the observed field and temperature dependence of the photocurrent in $\mathrm{P}\mathrm{P}\mathrm{V}\ensuremath{\mathbin:}\mathrm{P}\mathrm{C}\mathrm{B}\mathrm{M}$ blends. At room temperature only 60% of the generated bound electron-hole pairs are dissociated and contribute to the short-circuit current, which is a major loss mechanism in photovoltaic devices based on this material system.
- Published
- 2004