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Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE

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11/16<br />

Efficiency [%]<br />

FF [%]<br />

9.5<br />

9.0<br />

8.5<br />

8.0<br />

7.5<br />

7.0<br />

6.5<br />

6.0<br />

5.5<br />

5.0<br />

80<br />

75<br />

70<br />

65<br />

60<br />

55<br />

50<br />

Initial<br />

Stable<br />

400 300 nm 200 nm 140 nm<br />

initial<br />

stable<br />

400 nm 300 nm 200 nm 140 nm<br />

30<br />

25<br />

20<br />

15<br />

10<br />

20<br />

18<br />

16<br />

14<br />

12<br />

10<br />

8<br />

6<br />

Degradation [%]<br />

degradation [%]<br />

V oc [mV]<br />

J sc [mA/cm 2 ]<br />

910<br />

900<br />

890<br />

880<br />

870<br />

860<br />

850<br />

840<br />

830<br />

820<br />

810<br />

800<br />

15<br />

14<br />

13<br />

12<br />

11<br />

10<br />

initial<br />

stable<br />

400 nm 300 nm 200 nm 140 nm<br />

400 nm 300 nm 200 nm 140 nm<br />

Fig.15: Dependency of a-Si n-i-p solar cell parameters on absorber layer thickness; initial and stable<br />

values are denoted by squares and circles, respectively. Triangles refer to the relative degradation<br />

on the scale to the right. The cells are deposited on glass coated with LP-CVD ZnO.<br />

3.3.3 Micromorph tandem cells with textured intermediate reflector [Sod09]<br />

A particularity of the n-i-p configuration is that the deposition is started with the thick bottom cell.<br />

Fig.14 shows that the collision of growth fronts can result in pinched regions and eventually in the<br />

formation of defective material which is highlighted by the arrow the centre of the film shown in the left<br />

panel. Apart from this observation, the microcrystalline material normally tends to smooth out any existing<br />

structure which poses a challenge to the light trapping strategy for n-i-p tandem cells. For light<br />

trapping in the bottom cell the texture of the back reflector should be relatively large (in the order of 1<br />

to 1.5 µm). As such it will be already too large for light trapping in the amorphous top cell which works<br />

best with structures in the order of 300 nm, and additionally it is smoothened out by the growth of the<br />

bottom cell.<br />

In order to solve this dilemma, an asymmetrical intermediate reflector of LPCVD-ZnO was introduced.<br />

This material is known to develop its own intrinsic surface structure, almost independently of the substrate<br />

it grows on. This configuration allows a separation of the two different light trapping requirements;<br />

the bottom cell is grown on a well adapted substrate for microcrystalline cells like the 2D grating<br />

or a hot silver substrate. Then, the textured ZnO reflector is grown which delivers an ideal texture<br />

for the amorphous top cell which is identical to the case of the cells presented in Fig.15.<br />

Fig.16 shows the EQE and J-V characteristics of a tandem device on glass with initial efficiency of<br />

10.3% and a stabilized efficiency of 10.1%. Because all processes are kept compatible with processing<br />

on plastic substrates, it was also possible to apply the recipes to the flexible plastic substrate with<br />

the 2D grating structure. A corresponding device on plastic is shown in the separate report on the EU-<br />

Project Flexcellence and reaches 9.8% stabilised efficiency, with further space for improvement.<br />

initial<br />

stable<br />

41/290<br />

New processes and device structures for the fabrication of high efficiency thin film silicon photovoltaic modules, C. Ballif, University of Neuchâtel<br />

14<br />

12<br />

10<br />

8<br />

6<br />

4<br />

2<br />

4<br />

2<br />

0<br />

degradation [%]<br />

Degradation [%]

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