Abstract
Ideally pure single-crystal silicon shows an intrinsic electrical conductivity, which is low at room temperature and rises with increasing temperature. To produce devices, well-defined parts of the silicon specimen, usually in the form of a wafer, must exhibit a well-defined surplus of either negative (electrons) or positive (holes) carriers, leading to n-type conductivity or p-type conductivity, respectively. n-type conductivity is obtained by doping with donors such as P, As, and Sb, and p-type conductivity is obtained with acceptors such as B, Al, Ga, and In. Donor or acceptor atoms must be on substitutional sites in the single-crystal silicon lattice to be electrically active, i.e. to form levels close to the conduction band or close to the valence band, respectively. The particular cases of N in Si and C are discussed in the context of ion implantation.
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Krimmel, E.F. (2004). Defects, Diffusion, Ion Implantation, Recrystallization, and Dielectrics. In: Siffert, P., Krimmel, E.F. (eds) Silicon. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-09897-4_11
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DOI: https://doi.org/10.1007/978-3-662-09897-4_11
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