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Programm Photovoltaik Ausgabe 2008 ... - Bundesamt für Energie BFE

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Introduction<br />

Cyanine dyes were developed at the beginning of the 20 th century, mainly as sensitizers for silver halide<br />

emulsions in the photographic process. Above all, cyanines exhibit extraordinarly high extinction<br />

coefficients and tunable absorption spectra. Most interesting is the possibility to achieve strong light<br />

absorption in the near-infrared domain, which is presently thought to be one possibility to enhance<br />

power conversion efficiency of organic solar cells.<br />

Objectives<br />

So far only few works have studied thin solid cyanine films as active layers in solar cells. Simple<br />

bilayer heterojunction devices were fabricated, proving the concept of using cyanines as electron donors<br />

or acceptors. Unfortunately the power conversion efficiency has been typically around 0.1 % or<br />

lower, which is too modest for most applications. The cause of this poor performance has been unclear<br />

so far. This work highlights the importance of charge carrier transport in cyanine dye based solar<br />

cell [1].<br />

Work performed and results obtained<br />

When cyanine films were exposed to ambient atmosphere under white light irradiation, a steep rise of<br />

the conductivity of the film could be observed (Fig. 1). Clearly light is required to induce the conductivity<br />

increase. By separately investigating the effect of oxygen and water it could be demonstrated that<br />

both are needed for the doping process. Photochemical reactions of cyanine dyes with oxygen involve<br />

either energy transfer or electron transfer. While the former leads to reactive singlet oxygen, the latter<br />

-<br />

leads to the transient superoxide anion O2 species that further react with a neighboring cyanine molecule.<br />

Contrary to the energy transfer mechanism, the electron transfer mechanism produces a cationic<br />

cyanine species which can be regarded as positive charge carrier.<br />

Conductivity (S/cm)<br />

6.0x10 -4<br />

5.0x10 -4<br />

4.0x10 -4<br />

3.0x10 -4<br />

2.0x10 -4<br />

1.0x10 -4<br />

0.0<br />

white light irradiation<br />

dark<br />

0 5 10 15 20 25 30<br />

Exposure time to air (min)<br />

Fig. 1: Four probe conductivity measurement of a thin cyanine film as a function of exposure time to<br />

ambient atmosphere in the dark (black squares) and under white light irradiation (red squares).<br />

Cyanine – fullerene C60 bilayer solar cells were fabricated on transparent conducting glass coated by a<br />

conductive polymer interlayer (PEDOT:PSS). Photochemical doping of the cyanine film had a tremendous<br />

impact on the device performance. Most importantly the power conversion efficiency of the device<br />

increased from 0.14% to 1.2% which is among the best efficiencies for organic bilayer devices.<br />

The short circuit current increase from 0.46 mA/cm 2 to 1.83 mA/cm 2 as well as the fill factor improvement<br />

from 0.19 to 0.27 further emphasize the ameliorated charge transport due to the doping process.<br />

Seite 120 von 288<br />

Doping of cyanine solar cells: enhancing charge transport, B. Fan, F. Nüesch, Empa<br />

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