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218 BULK CRYSTAL GROWTH AND WAFERING FOR PV<br />

18<br />

Conventional mc-Si<br />

Freiberg mc-Si<br />

Mean grain size<br />

[mm 2 ]<br />

16<br />

14<br />

12<br />

10<br />

Block height<br />

[arbitr. units]<br />

Figure 6.9 Mean grain size as a function of the block height for conventional Bridgman-type<br />

multicrystalline silicon (mc-Si) and the faster crystallised block-cast material from the Freiberg<br />

production facility of Deutsche Solar GmbH. Reduced crystallisation times lead to slightly lower<br />

grain sizes of the Freiberg mc-Si<br />

Because also in modern high-throughput production processes a nearly perfectly planar<br />

solidification front is kept throughout the crystallisation process, grain boundaries show<br />

only weak electrical activities and therefore are generally considered as less important for<br />

solar cell efficiencies.<br />

Crystal dislocations, however, turned out to be the most efficiency-relevant defects<br />

in multicrystalline silicon for solar cells. The dislocation density that is experimentally<br />

accessible by counting micrometer-small etch pits after appropriate chemical etching steps<br />

nearly shows a perfect correlation to the wafer lifetime and diffusion length (Figure 6.10)<br />

that are closely linked to solar cell performance. Dislocations are induced and multiplied<br />

Wafer size<br />

5 × 5 cm 2<br />

4 5 6<br />

2.0 2.5 3.0<br />

Log dislocation density N d<br />

[cm −2 ]<br />

(a)<br />

Effective lifetime τ<br />

[µs]<br />

(b)<br />

Figure 6.10 Topographies of the dislocation density N d (a) and the effective lifetime τ eff (b) of<br />

a typical multicrystalline silicon wafer showing the excellent correlation of both parameters. The<br />

effective lifetime measurements were conducted out without any surface passivation and thus are<br />

limited to less than approximately 3 µs by surface recombination processes

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