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Essentially there are two "bands" in every material which
the electrons within the material may occupy - the valence band and the
higher-energy conduction band. Electrons in the valence band can be considered
as being bound in place, whereas electrons in the conduction band may
act as mobile charge carriers.
Conduction band
Valence band
Conduction band
Valence band
In dielectrics the two bands are separated by a certain
energy gap Eg, corresponding to energies that are forbidden
to the electrons.
Conduction band
(vacant)
Valence band
(occupied)
Since the valence band is lower in energy, electrons will
preferentially occupy this band. Therefore in a dielectric under normal
conditions, the conduction band will be empty.
Conduction band
(vacant)
Valence band
(occupied)
If an electron in the valence band is supplied with energy
greater than or equal to Eg, for example from a high-energy photon,
it may be promoted to the conduction band.
Conduction band
(vacant)
Valence band
(occupied)
An electric field of sufficient strength can supply enough
energy to promote many electrons to the conduction band at once. Since
electrons in the conduction band act as charge carriers, the material
now conducts charge rather than storing it.