Van Hove singularity
In condensed matter physics, a Van Hove singularity is a singularity (non-smooth point) in the density of states (DOS) of a crystalline solid.
The wavevectors at which Van Hove singularities occur are often referred to as critical points of the Brillouin zone.
For three-dimensional crystals, they take the form of kinks (where the density of states is not differentiable).
The most common application of the Van Hove singularity concept comes in the analysis of optical absorption spectra.
The occurrence of such singularities was first analyzed by the Belgian physicist Léon Van Hove in 1953 for the case of phonon densities of states.
The shortest wavelength needed to describe a wavemotion in the lattice is equal to 2a which then corresponds to the largest needed wave number
We may define the density of states g(k)dk as the number of standing waves with wave vector k to k+dk:[3] Extending the analysis to wavevectors in three dimensions the density of states in a box of side length
is a volume element in k-space, and which, for electrons, will need to be multiplied by a factor of 2 to account for the two possible spin orientations.
By the chain rule, the DOS in energy space can be expressed as where
The set of points in k-space which correspond to a particular energy E form a surface in k-space, and the gradient of E will be a vector perpendicular to this surface at every point.
[4] The density of states as a function of this energy E satisfies: where the integral is over the surface
is perpendicular to the surface and therefore parallel to the gradient of E. If the coordinate system is just a rotation of the original coordinate system, then the volume element in k-prime space will be We can then write dE as: and, substituting into the expression for g(E) we have: where the
term is an area element on the constant-E surface.
has an extremum, the integrand in the DOS expression diverges.
The Van Hove singularities are the features that occur in the DOS function at these
A detailed analysis[5] shows that there are four types of Van Hove singularities in three-dimensional space, depending on whether the band structure goes through a local maximum, a local minimum or a saddle point.
The function g(E) tends to have square-root singularities (see the Figure) since for a spherical free electron gas Fermi surface In two dimensions the DOS is logarithmically divergent at a saddle point and in one dimension the DOS itself is infinite where
The optical absorption spectrum of a solid is most straightforwardly calculated from the electronic band structure using Fermi's Golden Rule where the relevant matrix element to be evaluated is the dipole operator
The optical absorption is then essentially the product of the dipole operator matrix element (also known as the oscillator strength) and the JDOS.
The divergences in the two- and one-dimensional DOS might be expected to be a mathematical formality, but in fact they are readily observable.
Highly anisotropic solids like graphite (quasi-2D) and Bechgaard salts (quasi-1D) show anomalies in spectroscopic measurements that are attributable to the Van Hove singularities.
Van Hove singularities play a significant role in understanding optical intensities in single-walled carbon nanotubes (SWNTs) which are also quasi-1D systems.
Twisted graphene layers also show pronounced Van-Hove singularities in the DOS due to the interlayer coupling.
