Diffraction catastrophes and semiclassical quantum mechanics for Veselago lensing in graphene
arXiv:1703.07769 · doi:10.1103/PhysRevB.96.045305
Abstract
We study the effect of trigonal warping on the focussing of electrons by n-p junctions in graphene. We find that perfect focussing, which was predicted for massless Dirac fermions, is only preserved for one specific sample orientation. In the general case, trigonal warping leads to the formation of cusp caustics, with a different position of the focus for graphene's two valleys. We develop a semiclassical theory to compute these positions and find very good agreement with tight-binding simulations. Considering the transmission as a function of potential strength, we find that trigonal warping splits the single Dirac peak into two distinct peaks, leading to valley polarization. We obtain the transmission curves from tight-binding simulations and find that they are in very good agreement with the results of a billiard model that incorporates trigonal warping. Furthermore, the positions of the transmission maxima and the scaling of the peak width are accurately predicted by our semiclassical theory. Our semiclassical analysis can easily be carried over to other Dirac materials, which generally have different Fermi surface distortions.
6 pages, 4 figures, plus supplemental material. Important reference added and text updated
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Cited by in corpus (7)
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- Electronic optics in graphene in the semiclassical approximation
- Valley-dependent Lorentz force and Aharonov-Bohm phase in strained graphene p-n junction
- Perfect transmission at oblique incidence by trigonal warping in graphene P-N junctions
- Effectuating tunable valley selection via multi-terminal monolayer graphene devices
- Quantum Charged Spinning Massless Particles in 2+1 dimensions
- Two-dimensional Dirac matter in the semiclassical regime