Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
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So far, experiments were performed using one cyanine dye with a mobile counter ion (CyC, Fig. 1)<br />
and one dye with a bound counter ion (an internal salt). For the latter case, we concluded that van der<br />
Waals forces are responsible for film break-up, and the theoretical predictions for thickness ranges<br />
that result in stable, metastable or unstable films could be readily realized experimentally [5]. The<br />
situation was different for CyC where all films were unstable, although a stable layered configuration<br />
with PCBM wetting CyC would be expected from the surface tension values alone. From our analysis<br />
we concluded that van der Waals forces and convective flows during spin coating do not play a major<br />
role for structure formation. A characteristic of CyC is that the positively charged cyanine is associated<br />
by the mobile negative perchlorate counter ion (Fig. 1). This can give rise to electrostatic forces in thin<br />
films, and space charge can build up if the anions diffuse from the cyanine layer into the PCBM phase.<br />
The thermodynamic model reveals that the transfer of ions lowers the free energy of the system. Surface<br />
and interface fluctuations favour continuing ion transfer, which amplifies the film undulations and<br />
effectively destabilizes the film.<br />
Fig. 2: Atomic force microscopy images of PCBM/cyanine dye films coated on glass from solution. The<br />
as-prepared film morphology consisted of circular PCBM domains with surprisingly uniform sizes<br />
(right). The left panel displays the continuous matrix of the complementary cyanine dye material. The<br />
individual components were made visible by treating the film with selective solvents.<br />
We found that liquid-liquid dewetting results in a large variety of phase morphologies, with tuneable<br />
dimensions well below 100 nm (Fig. 2). Qualitatively, the resulting type of morphology depends on the<br />
ratio of the layer thicknesses, whereas the dominant wavelength of the domains is determined by the<br />
absolute film thickness. These are material independent parameters and, therefore, the patterning<br />
method is rather robust. In ongoing experiments, we study the quantitative aspects of the dewetting<br />
process and adapt the concept to other cyanine dyes.<br />
National / international collaborations<br />
Collaboration with J. Groenewold (Uni Utrecht, NL) “Nanoscale structuring of heterojunction ionic organic<br />
solar cells by liquid-liquid dewetting,” project submitted to “Polymol;” a FP6 financed PV ERA<br />
NET project.<br />
Collaboration with J.-E. Moser (EPFL), photophysics of cyanine dyes studied by fast spectroscopy.<br />
Collaboration with U. Steiner (Cambridge), fundamental aspects of thin-film destabilization, external<br />
forces as a means for film structuring.<br />
Organic photovoltaic devices, F. Nüesch,Empa<br />
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