valence band

This leaves an associated hole behind, in the valence band.

This is also applicable for holes in the valence band.

It is typically used to assess the valence band structure.

The vacuum can be seen as a special type of insulator without a valence band.

In metals, there are not enough electrons to fill the valence band completely.

Most of the states with low energy (closer to the nucleus) are occupied, up to the valence band.

Because the valence band is so nearly full, its electrons are not mobile, and cannot flow as electrical current.

Hole conduction in a valence band can be explained by the following analogy.

Then, the density of free carriers in the conduction and/or the valence band will increase.

In the valence band the mobile carriers are holes.

The valence band is the highest band where the electrons are not free to move.

The hole is an empty state that allows electrons in the valence band some degree of freedom.

This leaves a positive 'hole' in the valence band.

These parameters are very closely related to the effective masses of the holes in various valence bands.

Helium II has no such valence band but nevertheless conducts heat well.

The Fermi level can be calculated from the density of states in the conduction and valence bands.

To understand the concept of a valence band, it is important to consider the atomic structure of a metal first.

Most materials that conduct heat well have a valence band of free electrons which serve to transfer the heat.

The valence band offset is simply given by:

They "accept" electrons from the semiconductor's valence band.

Beginning immediately after being promoted, there is a chance that a given electron will recombine with a hole and move back into the valence band.

The valence band, immediately below the forbidden band, is normally very nearly completely occupied.

A full (or nearly full) valence band is present in semiconductors and Electrical insulations.

However, an electron needs a certain amount of energy to jump from a valence band to a conduction band.

At the Г-point in the band structure, and orbitals form valence bands.