4.8 Article

Impact of Acceptor Fluorination on the Performance of All-Polymer Solar Cells

Journal

ACS APPLIED MATERIALS & INTERFACES
Volume 10, Issue 1, Pages 955-969

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsami.7b14582

Keywords

all-polymer solar cells; planarization; fluorination; morphology; photophysics; GIWAXS; R-SoXS

Funding

  1. International Synchrotron Access Program (ISAP)
  2. Australian Government
  3. Australian Research Council [FT100100275]
  4. Rutherford Discovery Fellowship
  5. Office of Science, Office of Basic Energy Sciences, of the U.S. Department of Energy [DE-AC02-05CH11231]
  6. DFG [IRTG SOMAS 1642]

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Here, we systematically study the effect of fluorination on the performance of all-polymer solar cells by employing a naphthalene diimide (NDI)-based polymer acceptor with thiophene-flanked phenyl co-monomer. Fluorination of the phenyl co-monomer with either two or four fluorine units is used to create a series of acceptor polymers with either no fluorination (PNDITPhT), bifluorination (PNDITF2T), or tetrafluorination (PNDITF4T). In blends with the donor polymer PTB7-Th, fluorination results in an increase in power conversion efficiency from 3.1 to 4.6% despite a decrease in open-circuit voltage from 0.86 V (unfluorinated) to 0.78 V (tetrafluorinated). Countering this decrease in open-circuit voltage is an increase in short-circuit current from 7.7 to 11.7 mA/cm(2) as well as an increase in fill factor from 0.45 to 0.53. The origin of the improvement in performance with fluorination is explored using a combination of morphological, photophysical, and charge-transport studies. Interestingly, fluorination is found not to affect the ultrafast charge-generation kinetics, but instead is found to improve charge-collection yield subsequent to charge generation, linked to improved electron mobility and improved phase separation. Fluorination also leads to improved light absorption, with the blue-shifted absorption profile of the fluorinated polymers complementing the absorption profile of the low-band gap PTB7-Th.

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