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Abstract

The basic material of a field-effect transistor is a chemically pure and perfect single crystal of silicon. In such a crystal the atoms are ordered in a periodic pattern such that they are all lined up perfectly throughout the entire lattice. Silicon is a tetravalent element so that Si atoms sit at the apices and at the centre of tetrahedra in the lattice. Therefore a single crystal of silicon when seen from a particular direction appears as shown in figure 1.1. The electrical characteristics of such crystals are best described with the help of energy band models, tools derived from band theory.

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Further Reading

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© 1974 J. T. Wallmark and L. G. Carlstedt

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Wallmark, J.T., Carlstedt, L.G. (1974). Properties of Semiconductors. In: Field-Effect Transistors in Integrated Circuits. Palgrave, London. https://doi.org/10.1007/978-1-349-02053-9_2

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  • DOI: https://doi.org/10.1007/978-1-349-02053-9_2

  • Publisher Name: Palgrave, London

  • Print ISBN: 978-1-349-02055-3

  • Online ISBN: 978-1-349-02053-9

  • eBook Packages: EngineeringEngineering (R0)

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