The transparency of graphene and other direct-gap two dimensional materials
arXiv:1609.07571 · doi:10.1103/PhysRevB.94.205439
Abstract
Graphene and other two-dimensional materials display remarkable optical properties, including a simple light transparency of for light in the visible region. Most theoretical rationalizations of this "universal" opacity employ a model coupling light to the electron's crystal momentum and put emphasis on the linear dispersion of the graphene bands. However, such a formulation of interband absorption is not allowable within band structure theory, because it conflates the crystal momentum label with the canonical momentum operator. We show that the physical origin of the optical behavior of graphene can be explained within a straightforward picture with the correct use of canonical momentum coupling. Its essence lies in the two-dimensional character of the density of states rather than in the precise dispersion relation, and therefore the discussion is applicable to other systems such as semiconductor membranes. At higher energies the calculation predicts a peak corresponding to a van Hove singularity as well as a specific asymmetry in the absorption spectrum of graphene, in agreement with previous results.
APS PHYSICS Synopsis: http://physics.aps.org/synopsis-for/10.1103/PhysRevB.94.205439
References in corpus (6)
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- Measurement of the Optical Conductivity of Graphene
- Optical properties of graphene
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Cited by in corpus (4)
- Transmission of near-resonant light through a dense slab of cold atoms
- Optical absorption in two-dimensional materials with tilted Dirac cones
- Universal transparency and fine band structure near the Dirac point in HgTe quantum wells
- Sub-Sharvin conductance and incoherent shot-noise in graphene disks at magnetic field