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Damage formation and annealing studies of low energy ion implants ...

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abundance <strong>of</strong> 92.23 % (3). This has a small bearing on the MEIS spectra <strong>and</strong> is<br />

discussed in sect<strong>ion</strong> 4.2.2.<br />

Figure 3.1 Si unit cell. From (2).<br />

Figure 3.2 Si (100), (110) <strong>and</strong> (111) planes. From (3)<br />

Intrinsic (undoped) Si has a b<strong>and</strong> gap <strong>of</strong> 1.1 eV at room temperature <strong>and</strong> will<br />

have an equal (<strong>low</strong>) concentrat<strong>ion</strong> <strong>of</strong> holes <strong>and</strong> electrons (5). Extrinsic (doped) Si will<br />

have an excess <strong>of</strong> holes or electrons depending on the doping type. Usually doping is<br />

with group III <strong>and</strong> V atoms although group II <strong>and</strong> VI are also used. To be electrically<br />

active these atoms have to replace a Si atom being covalently bound to Si atoms,<br />

creating an unsatisfied bond (hole) if a group III <strong>ion</strong> or with an extra electron not<br />

involved in bonding, available <strong>of</strong> conduct<strong>ion</strong>, if group V dopant.<br />

Si oxidises in air to form a native SiO2 layer. This SiO2 is amorphous <strong>and</strong> is an<br />

electrical insulator. The native oxide can easily be removed in a HF dip. Thin oxide<br />

layers are used as the insulating gate oxide <strong>and</strong> can easily be grown on the surface <strong>of</strong> Si<br />

to the required thickness. Mechanisms for oxide growth are discussed in (6) <strong>and</strong><br />

references therein. Oxygen molecules react with surface Si atoms to form SiO2. Further<br />

growth is due to the diffus<strong>ion</strong> <strong>of</strong> oxygen through the SiO2 layer which reacts with Si at<br />

31

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