Basic Concepts
Any solid has a large number of bands. In theory, a solid can have infinitely many bands (just as an atom has infinitely many energy levels). However, all but a few of these bands lie at energies so high that any electron that attains those energies will escape from the solid. These bands are usually disregarded.
Bands have different widths, based upon the properties of the atomic orbitals from which they arise. Also, allowed bands may overlap, producing (for practical purposes) a single large band.
Figure 1 shows a simplified picture of the bands in a solid that allows the three major types of materials to be identified: metals, semiconductors and insulators.
Metals contain a band that is partly empty and partly filled regardless of temperature. Therefore they have very high conductivity.
The lowermost band is called the valence band by analogy with the valence electrons of individual atoms. This band is almost fully occupied in an insulator or semiconductor. The uppermost, almost unoccupied band is called the conduction band because only when electrons are excited to the conduction band can current flow in these materials. The difference between insulators and semiconductors is only that the forbidden band gap between the valence band and conduction band is larger in an insulator, so that fewer electrons are found there and the electrical conductivity is lower. Because one of the main mechanisms for electrons to be excited to the conduction band is due to thermal energy, the conductivity of semiconductors is strongly dependent on the temperature of the material.
This band gap is one of the most useful aspects of the band structure, as it strongly influences the electrical and optical properties of the material. Electrons can transfer from one band to the other by means of carrier generation and recombination processes. The band gap and defect states created in the band gap by doping can be used to create semiconductor devices such as solar cells, diodes, transistors, laser diodes, and others.
Read more about this topic: Electronic Band Structure
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