Abstract
Of the many options for broadly classifying solids, electrical resistivity has proved to be the most useful. The grouping of materials into insulators, semiconductors, semimetals, and metals involves a parameter with a range of order 1010. The resistivity boundaries between the classifications are not very sharp, but they are sharp enough to make the separation for most practical purposes. For the semiconductor regime, the resistivity is betwen 109 and 10−3 ohm -cm, but we will also discuss insulators with resistivities above 109 ohm-cm and doped semiconductors and semimetals with resistivities below 10−3 ohm-cm. The distinction at the boundary between semiconductors and insulators will be made on the basis of the size of the fundamental (minimum) band gap. Semiconductors are assumed to have band gaps from 0 to ∼4eV, insulators >4eV, and semimetals ≤0. Gray Sn (α-Sn) is an example of a borderline material which has zero band gap. It has been called a zero-gap semiconductor; it has also been called in ideal semimetal.
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References
C. Kittel: Introduction to Solid State Physics, 6th ed. (Wiley, New York 1986)
F. Bassani, G. Pastori Parravicini: Electronic States and Optical Transitions in Solids (Pergamon, Oxford 1975)
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© 1988 Springer-Verlag Berlin Heidelberg
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Cohen, M.L., Chelikowsky, J.R. (1988). Theoretical Concepts and Methods. In: Electronic Structure and Optical Properties of Semiconductors. Springer Series in Solid-State Sciences, vol 75. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-97080-1_2
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DOI: https://doi.org/10.1007/978-3-642-97080-1_2
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-97082-5
Online ISBN: 978-3-642-97080-1
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