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Silicon-based solar cells Characteristics and production processes ...

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<strong>Silicon</strong>-<strong>based</strong> <strong>solar</strong> <strong>cells</strong> – characteristics <strong>and</strong> <strong>production</strong> <strong>processes</strong><br />

acceptor, donor <strong>and</strong> trapping states. The effect of the surface on the kinetics of the<br />

electron <strong>processes</strong> is described by a quantity called surface recombination velocity S,<br />

defined as [47]:<br />

J<br />

= σ<br />

rυ<br />

r<br />

N<br />

r<br />

(14)<br />

q⋅<br />

∆n<br />

r<br />

S =<br />

e<br />

where: J r – density of the electron or hole current flowing to the surface, for maintaining<br />

the established state in which the excess charge carrier concentration in the volume<br />

equals Δn e ,<br />

N r – number of recombination centres per surface unit,<br />

σ r – collision cross-section of charge carrier capturing,<br />

υ r – thermal velocity of charge carriers,<br />

The surface recombination process taking place through defects is described by<br />

the Shockley-Read-Hall theory, according to which the recombination velocity<br />

increases with the increasing recombination centres N r or free charge carrier<br />

concentration on the surface [48]. The increase of the surface recombination directly<br />

affects the increase of the current I r , causing a drop of the voltage <strong>and</strong> the current<br />

possible to obtain from the cell [49]. That is why, on the surface of Si, thin layers<br />

of compounds are formed, whose atoms, combining with the surface semi-conductor<br />

atoms, complement their incomplete bondings, that is they passivize the surface. In<br />

practice, the surface passivation is realized through oxidization of the silicon plate<br />

surface in dry oxygen, at the temperature range of 800 o C ÷ 1100 o C. Another<br />

technique is coating the plate with a layer of hydrogenated silicon nitride with the<br />

method of plasma enhanced chemical vapour deposition (PECVD). The Si x N y :H layer,<br />

beside its passivating <strong>and</strong> protective effect on the Si-surface, is additionally<br />

advantageous in the fact that, during the high temperature metallization process<br />

of the front electrode, the hydrogen atoms released from the layer also passivize the<br />

material in its whole volume, which is a determining factor in the case of mc-Si <strong>cells</strong><br />

[50]. The silicon nitride layer deposited by means of PECVD allows for a passivation of<br />

the Si surface, but at the same time, it plays the role of an antireflection coating. The<br />

Si x N y :H layer, due to its electron affinity, is appropriate for the n-type Si. In the case of<br />

the p-type Si surface, more suitable seems to be an Al 2 O 3 layer, which is deposited<br />

with the method of ALD (Atomic Layer Deposition).<br />

25

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