Counter-propagating Fractional Hall states in mirror-symmetric Dirac semi-metals
arXiv:1711.05727 · doi:10.1103/PhysRevLett.121.066602
Abstract
The Landau bands of mirror symmetric 2D Dirac semi-metals (for example odd-layers of ABA-graphene) can be identified by their parity with respect to mirror symmetry. This symmetry facilitates a new class of counter-propagating Hall states at opposite but equal electron and hole filling factors ({\it m} odd). Here, we propose a Laughlin-like correlated liquid wavefunction, at the charge neutrality point, that exhibits fractionally charged quasi-particle/hole pair excitation of opposite parity. Using a bosonized one-dimensional edge state theory, we show that the longitudinal conductance of this state, , is robust to short-ranged inter-mode interactions.
4+ pages
References in corpus (8)
- Quantum Spin Hall Insulator State in HgTe Quantum Wells
- Electronic states and Landau levels in graphene stacks
- Chiral Decomposition in the Electronic Structure of Graphene Multilayers
- Evidence for a Spin Phase Transition at ν=0 in Bilayer Graphene
- Intra-Landau level Cyclotron Resonance in Bilayer Graphene
- The Effects of Landau level mixing on the fractional quantum Hall effect in monolayer Graphene
- New Dirac points and multiple Landau level crossings in biased trilayer graphene
- Tunable symmetries of integer and fractional quantum Hall phases in heterostructures with multiple Dirac bands