Fractional quantum Hall effects in graphene on a h-BN substrate
arXiv:1710.10786 · doi:10.7566/JPSJ.87.034708
Abstract
Fractional quantum Hall (FQH) effects in graphene are studied because of their relativistic characteristics and the valley degree of freedom. Recently FQH effects have been observed at various filling factors with graphene on a hexagonal boron nitride (h-BN) substrate. However, it is known that h-BN creates the mass term in the Dirac Hamiltonian that acts as the effective model of graphene. To understand recent experiments, we shall investigate many-body effects in the massive Dirac electron system. In this paper, we study the mass-term effects on the FQH states of Dirac electrons by exact diagonalization. We examine the ground state at filling factor 1/3 in the Landau level. Without the mass term, the ground state in the Laughlin state featuring valley degeneracy and the lowest excitation is characterized by the valley unpolarized state (known as the valley skyrmion state). Conversely, we find that the mass-term lifts the valley degeneracy due to the breaking of the inversion symmetry. We also demonstrate that the valley unpolarized excitation is suppressed and that the fully or partially polarized state appears in the lowest excitation by increasing the mass term. Finally, we discuss the stability of FQH states in the massive Dirac Hamiltonian in experimental situations. We find that our numerical results are in agreement with previous experimental results.
References in corpus (11)
- The electronic properties of graphene
- Boron nitride substrates for high-quality graphene electronics
- Multicomponent fractional quantum Hall effect in graphene
- Electronic properties of graphene hexagonal boron nitride moiré superlattice
- The Fractional Quantum Hall States of Dirac Electrons in Graphene
- Fractional Quantum Hall Effect in Graphene
- Composite Fermions and Broken Symmetries in Graphene
- Spontaneous polarization of composite fermions in the Landau level of graphene
- Coupled charge and valley excitations in graphene quantum Hall ferromagnets
- Relativistic Landau Models and Generation of Fuzzy Spheres
- Formulation of the Relativistic Quantum Hall Effect and "Parity Anomaly"