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Complete Report - University of New South Wales

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In silicon wafers that have naturally occurring defects, such as dislocations, grain boundaries<br />

and chemical impurities, the choice <strong>of</strong> wafer doping type can play a key role in mitigating<br />

the effect that the impurities have on the electrical quality <strong>of</strong> the wafer. For example, Figure<br />

4.3.2.1a shows the predicted injection-dependent normalized recombination rate for two<br />

Shockley-Read-Hall (SRH) defect species in p-type and n-type materials. Curves A and B<br />

predict the behaviour in p-type material: (A) for a defect located at a single energy level within<br />

the bandgap and (B) the behaviour for a defect distributed over a continuum <strong>of</strong> energy levels<br />

within the bandgap. Curve C predicts the behaviour for the same defects in n-type material,<br />

while curve D predicts the behaviour <strong>of</strong> both n-type and p-type material in the absence <strong>of</strong><br />

the defect. When viewed along the 1-sun operating loci (“1-sun Vmp”), it is clear that for a<br />

given defect species, the effective recombination rate depends signifi cantly on the doping<br />

type <strong>of</strong> the wafer. In this case, the recombination in the n-type wafer is one or two orders <strong>of</strong><br />

magnitude lower than the p-type wafer.<br />

Figure 4.3.2.1: (a) Predicted injection-dependent normalized recombination rate for n-type<br />

and p-type silicon wafers in the presence or absence <strong>of</strong> SRH defects; (b) Predicted effect <strong>of</strong><br />

SRH defects on the illuminated IV curve for the cases presented in (a).<br />

The signifi cance <strong>of</strong> the SRH behaviour in n-type and p-type wafers is highlighted in Figure<br />

4.3.2.1b, which shows the predicted illuminated IV curve for the four cases shown in Figure<br />

4.3.2.1a. The strong SRH recombination behaviour degrades the IV performance in the p-<br />

type material signifi cantly, reducing the operating point voltage by as much as 120 mV. The IV<br />

performance is hardly affected in the n-type material.<br />

The DSBC solar cell design, shown in Figure 4.3.2.2a, is ideal for making a direct comparison<br />

<strong>of</strong> solar cell terminal characteristics <strong>of</strong> solar cells made side-by-side on n-type and p-type<br />

silicon wafers. The DSBC processing sequence can be applied to either p-type or n-type<br />

wafers without signifi cant changes in the processing sequence - diffusions, oxidations, even<br />

metallisation processes can be applied with good effect to both types <strong>of</strong> wafers processed in<br />

split batches. Also, the DSBC process uses a heavy boron contact diffusion that is known to<br />

introduce diffusion induced misfi t dislocations into the bulk <strong>of</strong> the wafer. Such misfi t dislocations<br />

behave similarly to the SRH defects used in the simulations <strong>of</strong> Figure 4.3.2.1a. Figure 4.3.2.1b<br />

shows a comparison <strong>of</strong> terminal characteristics <strong>of</strong> p-type and n-type DSBC solar cells that<br />

were fabricated using the nearly identical fabrication sequences and processed in a split<br />

batch.<br />

34

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