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

that is, below approximately 10 12 /cm 3 . The importance of metal impurities for multicrystalline<br />

silicon solar cells is, however, based on metal impurities controlling the activity<br />

of extended defects, specifically that of crystal dislocations.<br />

We anticipate that metallic impurities are, for example, responsible for the observed<br />

systematic changes of the lifetime of multicrystalline silicon wafers after high-temperature<br />

steps in the range of 800 to 1000 ◦ C (e.g. the phosphorous diffusion step for fabrication<br />

of the solar cell pn-junction). The wafer lifetime quite commonly decreases in annealing<br />

steps above 900 ◦ C, where this decrease is even more significant at enhanced cooling<br />

speeds after the anneal. The proposed mechanism behind this lifetime degradation is a<br />

release of metal atoms from extended defects like dislocations into the wafer bulk material<br />

and a subsequent quenching of the metal atoms as highly recombinative point defects.<br />

Another hint of an extensive interaction between extended defects and metal<br />

impurities is given in Figure 6.13 that depicts the theoretical segregation profile of iron<br />

in an intentionally contaminated multicrystalline ingot (mean iron concentration: 7.9 ×<br />

10 17 /cm 3 ) as compared to the experimental one. We clearly can state a reduced experimentally<br />

determined segregation effectiveness most probably caused by iron segregation<br />

into extended defects competing with the segregation process in the liquid silicon phase<br />

during crystallisation.<br />

In order to prevent such defect–metal interaction processes leading to enhanced<br />

recombination activity, a very effective segregation of metallic impurities into the ingot<br />

top region has to be assured. This segregation effectiveness, however, decreases with both<br />

increasing crystallisation speed and increasing concentration of extended defects.<br />

1E + 20<br />

Fe segregation<br />

Concentration<br />

[1/cm 1 ]<br />

1E + 18<br />

1E + 16<br />

1E + 14<br />

1E + 12<br />

Segregation in<br />

crystal defects (?)<br />

Experiment<br />

Theory<br />

0 50 100 150<br />

Block height<br />

[mm]<br />

Diffusion<br />

during cooling<br />

Average Fe<br />

concentration:<br />

7.9 × 10 17 /cm 3<br />

Figure 6.13 Experimentally determined iron concentration of an intentionally contaminated multicrystalline<br />

silicon test ingot (mean Fe concentration: 7.9 × 10 17 /cm 3 ). The experimental data is<br />

given as a function of the block height and in comparison to the theoretically expected profile. The<br />

much higher than theoretically predicted concentration in the bottom and middle part of the ingot<br />

is attributed to a segregation not only into the silicon melt but also into extended crystal defects<br />

during solidification

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