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

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5/5<br />

Current density / mA.cm -2<br />

100<br />

80<br />

60<br />

40<br />

20<br />

0<br />

-20<br />

�=4.1%<br />

FF=51.1%<br />

J =28.5 mA/cm sc 2<br />

V =284 mV<br />

oc<br />

Area=0.6cm 2<br />

-40<br />

-0.6 -0.4 -0.2 0.0 0.2 0.4 0.6<br />

Voltage / V<br />

Figure 3: Current-Voltage curve of the solar cell with the highest efficiency so far of the performed<br />

experiments.<br />

One of the weaknesses cited for the Clevite process was that defects in the CdS layer caused preferential<br />

diffusion and led to localised inhomogeneities in the Cu2S layer. However, the high diffusion<br />

coefficient of Cu in In2Se3 at elevated temperatures [5] should reduce this effect significantly.<br />

Evaluation of 2007 and perspectives for <strong>2008</strong><br />

The low-temperature incorporation of Cu into In2Se3 layers by ion-exchange from aqueous solution<br />

was reported. This process results in thin films with a graded composition containing the crystalline<br />

phases �-Cu2-xSe and �-In2Se3. Annealing the films in the presence of Se vapour formed chalcopyrite<br />

CuInSe2 and homogenised the depth profile of the films. The results demonstrate a potential lowtemperature<br />

route to the formation of a precursor structure for CuInSe2 thin films. However, the ionexchange<br />

solution was destructive to the Mo back contact and attempts to use alternative contacts<br />

resulted in no incorporation of Cu into the In2Se3 films. The obtained layers are free of oxygen and<br />

carbon impurities and do not show any evidence of detrimental binary chalcogenide phases after the<br />

annealing step in selenium vapour.<br />

Further work is required to determine the reaction kinetics of the process and develop an improved<br />

solution in which the contact to the In2Se3 is stable. The reaction kinetics of the precursor film to the<br />

CIGS compound contains several phase transitions which may have positive and negative influences<br />

on the final CIGS properties.<br />

References<br />

[1] AM. Gabor, JR. Tuttle, DS. Albin et al. High Efficiency CuInxGa1-xSe2 Solar-Cells made from (Inx,Ga1-x)2Se3 precursor<br />

films, Applied Physics Letters 65 (2), 198-200, 1994<br />

[2] MA. Contreras, K. Ramanathan, et al. Diode characteristics in state-of-the-art ZnO/CdS/Cu(In(1-x)Gax)Se2 solar cells<br />

Progress in Photovoltaics 13, 209-216, 2005<br />

[3] J. Kessler, D. Schmid, S. Zweigart, H. Dittrich, HW. Schock, CuInSe2 film formation from sequential deposition of<br />

In(Se):Cu:Se, 12th European Photovoltaic Solar Energy Conference (1994) 648-652.<br />

[4] A. Ali, NA. Shah, AKS. Aqili, A. Maqsood, Investigation of Cu-containing low resistivity CdTe thin films deposited by<br />

the two-source evaporation technique, Semiconductor Science and Technology 21 (2006) 1296-1301,<br />

[5] K. Djessas, S. Yapi, G. Masse, et al. Diffusion of Cu, In, and Ga in In2Se3/CuGaSe2/SnO2 thin film photovoltaic structures,<br />

Journal of Applied Physics 95 (8): 4111-4116, 2004<br />

Thin Film CIGS Solar Cells with a Novel Low Cost Process, A. N. Tiwari, ETHZ Seite 87 von 288

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