density of states

The density of states at the Fermi level does not play a special role.

These states are numerous and therefore have a high density of states.

For crystals the electronic band structure determines the density of states.

The density of states depends on the dimensionality of the space.

This capacitance was defined through standard density of states in the solids.

The integral with respect to is given by the joint density of states for the two-D band.

Then g(E) is called the density of states if the energy spectrum is continuous.

Specific heat measurements give information about the low-energy density of states, which can be compared to theoretical models.

The metal contacts are characterized by a constant density of states, filled up to the Fermi energy.

The density of states as a function of this energy E is:

This temperature depends on the mass of the fermions and the energy density of states.

This makes density of states calculations of absorption band shapes easier.

This is determined by the density of states of phonons and photons.

The density of states is dependent upon the dimensional limits of the object itself.

The density of states plays an important role in the kinetic theory of solids.

In a semiconductor with an arbitrary density of states the Einstein relation is:

The biggest problem in performing a multicanonical ensemble is that the density of states has to be known a priori.

To calculate the density of states we rewrite equation (1) as follows:

The method performs a non-markovian random walk to build the density of states by quickly visiting all the available energy spectrum.

Computer simulations offer a set of algorithms to evaluate the density of states with a high accuracy.

A semimetal thus has no band gap and a negligible density of states at the Fermi level.

As the kubo gap increases there is also a decrease in the density of states located at the Fermi level.

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

Parallel tempering, for instance, the density of states is obtained as the main product of the simulation.

This feature allows to compute the density of states of systems with very rough energy landscape such as proteins.