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Complete Report - University of New South Wales

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Silicon Nitride Passivation <strong>of</strong> Bare, n-type Silicon Surfaces<br />

Figure 4.3.2.12 shows the effective surface recombination velocity (SRV) versus injection level<br />

curves for three different refractive index fi lms on FZ wafers. For comparison purpose, the<br />

effective SRV <strong>of</strong> a sample that had a 100 ohm/sq phosphorus diffusion and oxidation are<br />

also plotted on the same graph. The two dotted lines on the graphs that cross the effective<br />

SRV curves represent the locus <strong>of</strong> the 1-sun open-circuit voltage and approximate maximumpower<br />

voltage operating points for a high-effi ciency, 200-micron thick solar cell.<br />

As illustrated in the graph, the surface passivation quality <strong>of</strong> as-deposited SiN is exceptional,<br />

achieving better recombination than the baseline phosphorus diffused and oxidized surface.<br />

In our work, silicon-rich fi lms give the best surface passivation at as-deposited conditions.<br />

Table 4.3.2.2 summarizes the extracted SRV and implied open<br />

circuit voltages for various as-deposited silicon nitride fi lms.<br />

Figure 4.3.2.12: The effective surface recombination velocity vs.<br />

minority carrier density plots <strong>of</strong> various SiN on 1 ohm.cm n-type FZ<br />

wafer.<br />

Table 4.3.2.2: The best effective SRV, effective SRV at 1-sun Voc, and<br />

implied voltage at 1-Sun Voc operating points <strong>of</strong> various SiN fi lms on<br />

planar n-type surface <strong>of</strong> a 200-micron thick wafer.<br />

Refractive index Wafer type Best SRVeff (cm/s) SRVeff at Voc (cm/s) Imp Voc (mV)<br />

2.00 n-FZ 7.01 13.34 723<br />

2.35 n-FZ 2.29 10.74 732<br />

2.75 n-FZ 1.96 9.53 739<br />

Phos and oxide n-FZ 5.23 15.48 709<br />

A voltage test structure device was prepared to further demonstrate the exceptional<br />

passivation quality provided by our SiN fi lms on n-type wafers. The device has two very small<br />

diffused contact regions, one was phosphorus diffused and the other boron diffused. A lowindex<br />

(nr = 2.00) SiN fi lm was deposited on both sides <strong>of</strong> the wafer in the as-deposited condition.<br />

Small openings made photolithographically in the contact regions allowed the measurement<br />

<strong>of</strong> the open-circuit voltage at approximately 1-sun, 25ºC <strong>of</strong> 719 mV. Further improvement<br />

is expected during 2006, with open-circuit voltages approaching 725 mV expected for test<br />

structures and 700 mV in fully fabricated silicon nitride passivated solar cells.<br />

Silicon Nitride Passivation <strong>of</strong> Boron Diffused Emitters<br />

42<br />

The ability <strong>of</strong> silicon nitride to passivate a boron-diffused emitter is important for making higheffi<br />

ciency n-type silicon solar cells. Our results show that for some diffusion sheet resistances,<br />

boron diffusion process, and subsequent thermal treatment, SiN is particularly well-suited for<br />

passivating boron-diffused surface on n-type silicon. Figure 4.3.2.13a shows the implied open<br />

circuit voltages (extracted from photoconductance measurements) <strong>of</strong> various passivation<br />

fi lms on boron-diffused emitters with sheet resistances ranging from roughly 45 ohm/sq to<br />

250 ohm/sq, including silicon dioxide and various silicon nitride fi lms. The results illustrate<br />

that at the as-deposited condition for the sheet resistance range studied in this work, SiN<br />

provides poorer passivation compared to silicon dioxide. Interestingly, it appears that, at the<br />

as-deposited condition, the three different SiN fi lms provide roughly the equivalent passivation<br />

quality and have similar trend across the range <strong>of</strong> sheet resistances studied.

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