CHM 401



Properties: not as hard as metals, lower mp and bp but still solids, not ductile or malleable, poor electrical conductors - in many ways like a bad metal!

How do we explain this in terms of bonding?

Band theory but with more basis orbitals : require two bands, one filled and one empty

If the band gap is large enough, the material is an insulator because no metal-like properties arise from a filled band

If the band gap is on the order of thermal energies (small), then excitations of electrons from the valence band into the conduction band occurs

σ = neμ where (Boltzmann population of the conduction band)

μ has the same properties as in a metal but the Boltzmann term dominates so the conductivity of a semiconductor increases with increasing temperature

Doping of Semiconductors

Case 1 : the impurity has a filled orbital in the semiconductor band gap

Charge carries are created thermally (T > 0) by excitation from the filled impurity orbital into the conduction band. The population of the valence band is undisturbed; since it is filled, no charge can be transported through the valence band. The dopant is a species with more valence electrons than the semiconductor.

This is an n-type semiconductor.

Case 2. the impurity has an empty orbital in the band gap

At T > 0, the valence band is depopulated thermally creating charge carriers in the valence band (the electrons in the impurity orbital are not mobile, they are too far apart). The dopant must have fewer valence electrons than the semiconductor.

This is a p-type semiconductor

Semiconductor devices

Bonding properties at interfaces are the key to semiconductor device applications:

Electrons flow in one direction - from n-type to p-type

Under depicted conditions there is no electron flow – the electrons get trapped in the p-type device. Adding a potential to the p-type semiconductor, effectively populating the conduction band, can turn on electron flow.