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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3/6<br />
small and big particles that composes the DSL 18NR-AO paste as a main result of an increase in the<br />
fill factor. From an optical point of view, we have demonstrated that the use of DSL 30NRD-T + DSL<br />
18NR-AO allows preventing light loss within the photo-anode as a consequence from tangent light<br />
scattering [6].<br />
Efficiency (%)<br />
11<br />
10.5<br />
10<br />
9.5<br />
9<br />
0.5 sun<br />
1sun<br />
0.1 sun<br />
10.19<br />
10.00<br />
9.81<br />
10.57<br />
10.43<br />
10.32<br />
10.49<br />
10.35<br />
10.01<br />
10.79<br />
10.74<br />
10.61<br />
10.63<br />
10.44<br />
10.30<br />
9.93<br />
9.68<br />
9.50<br />
EPFL/CCIC EPFL/AO 18NR-T/AO 30NRD/AO Trans/AO AO<br />
Figure 1: Evolution of the conversion efficiency under different incident light intensity as a function of<br />
the different paste studied. (note that spot electrodes of ca. 0.283cm² were herein used and masked<br />
with an aperture of 0.159cm²).<br />
2) Optimization of the photo-voltaic characteristic of C101 dye<br />
The optimization of the photo-anode configuration obtained in accordance with the photo-physical<br />
properties of the C101 dye, we investigated a way to improve the monolayer characteristics. Pressure<br />
and temperature of sensitization are two parameters that govern the adsorption equilibria constant as<br />
well as the kinetic of adsorption. In the term of this first year project, we evaluated the influence of the<br />
temperature of sensitization of the C101 dye at three different temperatures: 60°C, 20°C and 4°C.<br />
Figure 2 shows the evolution of the photo-voltage, photo-current density, fill factor and photon-toelectron<br />
conversion efficiency as a function of the temperature which the cell has been sensitized.<br />
The temperature drastically influences the dye photovoltaic performance. Interestingly, the Voc of the<br />
cell can be tuned linearly from 714 mV, 752 mV to 768 mV in respect to a gradual temperature decrease<br />
from 60°C, 20°C to 4°C, respectively. This comes in turn with a remarkable improvement of<br />
the fill factor from 0.708 to 0.725 while the short circuit current density of the cells slightly increases<br />
from 19.9 mA/cm² to 20.5 mA/cm². A similar tendency was also experienced at lower incident light<br />
intensity, although the gap between the values becomes narrower. As a result from the increase of<br />
the three cell characteristics, the low temperature sensitization approach affords a noteworthy enhancement<br />
in the photon-to-electron conversion efficiency from 10.1 %, 10.9 % to 11.5 %.<br />
Photo-voltage (mV)<br />
770<br />
760<br />
750<br />
740<br />
730<br />
720<br />
710<br />
0 10 20 30 40 50 60<br />
Grafting temperature (°C)<br />
21<br />
20.5<br />
20<br />
19.5<br />
19<br />
Photo-current Photo-current density (mA/cm²)<br />
Fill Factor<br />
0.73<br />
0.725<br />
0.72<br />
0.715<br />
0.71<br />
0.705<br />
0 10 20 30 40 50 60<br />
Grafting temperature (°C)<br />
Fig. 2: Evolution of the cell characteristics (Voc, Jsc, F.F. and �) as a function of the grafting temperature<br />
at 1 sun equivalent light intensity (A.M. 1.5G). The values indicated correspond to an average<br />
value obtained by repetition of the cells. Square cells dimension were 0.152 cm² and masked with an<br />
aperture 1mm larger than the photo-anode.<br />
Robust DSC, M. Graetzel, EPFL<br />
123/290<br />
12<br />
11.5<br />
11<br />
10.5<br />
10<br />
9.5<br />
Conversion efficiency (%)