Confined Dirac Particles in Constant and Tilted Magnetic Field
arXiv:1202.5226 · doi:10.1142/S0219887815500620
Abstract
We study the confinement of charged Dirac particles in 3+1 space-time due to the presence of a constant and tilted magnetic field. We focus on the nature of the solutions of the Dirac equation and on how they depend on the choice of vector potential that gives rise to the magnetic field. In particular, we select a "Landau gauge" such that the momentum is conserved along the direction of the vector potential yielding spinor wavefunctions, which are localized in the plane containing the magnetic field and normal to the vector potential. These wave functions are expressed in terms of the Hermite polynomials. We point out the relevance of these findings to the relativistic quantum Hall effect and compare with the results obtained for a constant magnetic field normal to the plane in 2+1 dimensions.
10 pages
References in corpus (6)
- Unconventional Integer Quantum Hall effect in graphene
- Landau level spectroscopy of ultrathin graphite layers
- Infrared spectroscopy of Landau levels in graphene
- Multi-carrier Transport in Epitaxial Multi-layer Graphene
- Energy spectrum of graphene multilayers in a parallel magnetic field
- Experimental review of graphene