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Surface and bulk passivation of multicrystalline silicon solar cells by ...

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5<br />

Figure 1.2 A schematic <strong>of</strong> photogeneration effect.<br />

In order to produce a <strong>solar</strong> cell, the semiconductor has to be contaminated or<br />

doped. Pure semiconductors (also called "intrinsic") do not conduct electricity at<br />

room temperature <strong>and</strong> are thus not useful for the fabrication <strong>of</strong> electronic devices.<br />

Semiconductors conduct electricity if they are doped with a small amount <strong>of</strong> impurity<br />

atoms. In the case <strong>of</strong> <strong>silicon</strong> (Si), these would be atoms from group III <strong>and</strong> group V<br />

<strong>of</strong> the periodic table. Impurities in semiconductors are divided into two broad<br />

categories: donors <strong>and</strong> acceptors. A donor is an element with typically one more<br />

valence electron than the group IV semiconductor. Each Si atom has four electrons in<br />

its outermost shell; these electrons are involved in forming chemical bonds with the<br />

neighboring Si atoms. For example, an arsenic (As) atom has five electrons in its<br />

outermost shell. The extra electron in As can be easily removed from the As donor on<br />

which it was originally localized. If this happens, the electron can move freely in the<br />

semiconductor material <strong>and</strong> conduct electric current. A semiconductor doped with<br />

donors is known as n-type material. An acceptor is an element with typically one<br />

fewer valence electron than the element that forms the semiconductor. A boron (B)<br />

atom has three electrons in its outermost shell. The missing electron in the chemical

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