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98 THE PHYSICS OF THE SOLAR CELL<br />

0.90<br />

4.0<br />

0.85<br />

FF<br />

0.80<br />

3.8<br />

0.75<br />

3.6<br />

V OC<br />

[V], FF<br />

0.70<br />

I SC<br />

I SC<br />

[A]<br />

0.65<br />

3.4<br />

0.60<br />

0.55<br />

V OC<br />

3.2<br />

0.50<br />

3.0<br />

10 0 10 1 10 2 10 3 10 4 10 5 10 6 10 7<br />

S BSF<br />

[cm/s]<br />

Figure 3.18 Effect of the back-surface field recombination velocity on solar cell performance. All<br />

other parameters are from Table 3.2<br />

Table 3.3<br />

No grid (s = 0)<br />

Full grid (s = 1)<br />

Special cases of S F,eff<br />

S F,eff = S F<br />

S F,eff →∞<br />

Dark (G = 0)<br />

Short circuit (V = 0)<br />

Vlarge(≈V OC )<br />

S F,eff = S F + sD p /W N<br />

1 − s<br />

S F,eff = S F<br />

S F,eff = S F + sD p /W N<br />

1 − s<br />

3.4.8 An Analogy for Understanding Solar Cell Operation:<br />

A Partial Summary<br />

The following analogy illustrates the importance of minimizing all sources of recombination<br />

in the solar cell. 4 Imagine a funnel that has a variety of holes of different shapes<br />

and sizes in it. It also has a stopcock at the bottom for controlling the flow of liquid<br />

4 This analogy was developed on the basis of discussions with Professor Richard J. Schwartz of Purdue University,<br />

West Lafayette, Indiana.

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