Electron-solid and electron-liquid phases in graphene
arXiv:1601.07130 · doi:10.1103/PhysRevB.93.155141
Abstract
We investigate the competition between electron-solid and quantum-liquid phases in graphene, which arise in partially filled Landau levels. The differences in the wave function describing the electrons in the presence of a perpendicular magnetic field in graphene with respect to the conventional semiconductors, such as GaAs, can be captured in a form factor which carries the Landau level index. This leads to a quantitative difference in the electron-solid and -liquid energies. For the lowest Landau level, there is no difference in the wave function of relativistic and non-relativistic systems. We compute the cohesive energy of the solid phase analytically using a Hartree-Fock Hamiltonian. The liquid energies are computed analytically as well as numerically, using exact diagonalization. We find that the liquid phase dominates in the n=1 Landau level, whereas the Wigner crystal and electron-bubble phases become more prominent in the n=2 and n=3 Landau level.
11 pages, 7 figures
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Cited by in corpus (6)
- Even denominator fractional quantum Hall states in higher Landau levels of graphene
- Competing Fractional Quantum Hall and Electron Solid Phases in Graphene
- Unconventional fractional quantum Hall states and Wigner crystallization in suspended Corbino graphene
- Anomalous Hall Crystals in Rhombohedral Multilayer Graphene II: General Mechanism and a Minimal Model
- Competition between fractional quantum Hall liquid and electron solid phases in the Landau levels of multilayer graphene
- Charge density waves and their transitions in anisotropic quantum Hall systems