Graphene is a single layer of carbon atoms densely packed in a honeycomb lattice. The energy structure of crystals depends on the interactions between orbitals in the lattice. The tight binding approximation (TB) neglects interactions between atoms separated by large distances—an approximation that greatly simplifies the analysis. In solid-state physics, the TB model [1] calculates the electronic band structure using an approximate set of wavefunctions constructed by superposition of localized atomic orbitals.
This Demonstration calculates and plots the tight-binding (TB) electronic band structure of graphene as the 2D hexagonal carbon crystal. The band structure of graphene is obtained from the TB approximation including only first-nearest-neighbor carbon-carbon interactions of
-orbitals of a single honeycomb graphite sheet. This is given by a simple analytical relation, derived by diagonalization of the
Bloch Hamiltonian for the diatomic graphene unit cell [2]:
, with
,
with the phase factor
.
In this expression,
is the TB hopping parameter (overlap integral between
-orbitals),
is the on-site energy parameter,
is the overlap parameter,
is the lattice parameter of graphene, the
and
indices stand for valence and conduction bands, respectively, and
represents the 2D wavevector components along the
and
directions in the 2D Brillouin zone of graphene. The parameters
and
are expressed in electron-volt units (eV), whereas
is given in nondimensional units. At the special points
and
of the graphene BZ the valence and conduction bands cross at the Fermi level (energy at 0 eV).
The traditional presentation of an electronic dispersion along the
lines in Brillouin zone is given by selecting "usual" under "show Brillouin zone". Checking "show mesh" gives the distribution of allowed states inside the bands representing the density of states function. Check "add BZ and points" to see the location of high-symmetry points in BZ.
Setter bars under "show more detailed dispersion" let you compare the lattice electron behavior at the hyperbolic saddle
-point and quasi-linear (Dirac) dispersion curves at the
-points of BZ.
Snapshot 1: traditional representation of an electronic dispersion relation for the graphene along the
lines of the first Brillouin zone
Snapshot 2: pseudo-3D energy dispersion for the two
-bands in the first Brillouin zone of a 2D honeycomb graphene lattice
Snapshot 3: constant energy contours for the
-valence band and the first
Brillouin zone of the graphene
Snapshot 4: same constant energy contours for the
-conduction band in an extended
Brillouin zone
Snapshot 5: pseudo-3D energy dispersion for the
-conduction band at the saddle
-point (van Hove saddle point)
Snapshot 6: pseudo-3D near-linear energy dispersion for the two
-bands near
-points (Dirac electrons)
[1] C. Kittel,
Solid State Physics, Hoboken, NJ: John Wiley and Sons, Inc., 1996.
[2] R. Saito, G. Dresselhaus, and M. S. Dresselhaus,
Physical Properties of Carbon Nanotubes, London: Imperial College Press, 1998.
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