4.2 Article

Charge generation dynamics in polymer/polymer solar cells studied by transient absorption spectroscopy

Journal

JOURNAL OF PHOTONICS FOR ENERGY
Volume 1, Issue -, Pages -

Publisher

SPIE-SOC PHOTO-OPTICAL INSTRUMENTATION ENGINEERS
DOI: 10.1117/1.3569105

Keywords

polymer/fullerene solar cell; polymer/polymer solar cell; charge generation; polaron; transient absorption spectroscopy; phase separation

Funding

  1. JST PRESTO program (Photoenergy and Conversion Systems and Materials for the Next-Generation Solar Cells) from the Ministry of Education, Culture, Sports, Science, and Technology, Japan
  2. Global COE program (International Center for Integrated Research and Advanced Education in Materials Science) from the Ministry of Education, Culture, Sports, Science, and Technology, Japan

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Currently, polymer/fullerene solar cells have significantly higher power conversion efficiency than polymer/polymer solar cells. In order to address the origin of this wide gap, we measured the transient absorption spectra of polymer/polymer blend films based on poly(3-hexylthiophene) (P3HT) and poly(9,9-dioctylfluorene-alt-benzothiadiazole) (F8BT), and analyzed the charge generation dynamics in comparison with that of a polymer/fullerene blend film based on P3HT and [6,6]-phenyl-C-61 butyric acid methyl ether (PCBM). In P3HT/PCBM blend films, half of the polarons are generated immediately after pulsed laser excitation at the P3HT absorption band and the other half are generated with a rise constant of similar to 10 ps. The prompt polaron formation is assigned to the charge generation from P3HT singlet excitons located near the P3HT/PCBM interface and the delayed polaron formation to the charge generation after the exciton migration to the P3HT/PCBM interface. In P3HT/F8BT, on the other hand, F8BT singlet excitons observed immediately after the laser excitation decayed in a picosecond and P3HT singlet excitons increased on the same time constant, suggesting efficient energy transfer from F8BT to P3HT. Polymer polarons were generated on a time scale of similar to 40 ps, some of which were observed on a microsecond timescale but the yield was much smaller than that in P3HT/PCBM. We discuss the difference in charge generation dynamics in terms of kinetics and interfacial structures. (C) 2011 Society of Photo-Optical Instrumentation Engineers (SPIE). [DOI: 10.1117/1.3569105]

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