Hall Crystal States at and Moderate Landau Level Mixing
arXiv:cond-mat/0003459 · doi:10.1103/PhysRevLett.85.1954
Abstract
The quantum Hall state at low Zeeman coupling is well-known to be a translationally invariant singlet if Landau level mixing is small. At zero Zeeman interaction, as Landau level mixing increases, the translationally invariant state becomes unstable to aninhomogeneous state. This is the first realistic example of a full Hall crystal, which shows the coexistence of quantum Hall order and density wave order. The full Hall crystal differs from the more familiar Wigner crystal by a topological property, which results in it having only linearly dispersing collective modes at small , and no magnetophonon. I present calculations of the topological number and the collective modes.
Final version to appear in PRL. Two references added, minor changes to figures and text
References in corpus (1)
Cited by in corpus (12)
- Theory of Nematic Fractional Quantum Hall State
- Hamiltonian theory of fractionally filled Chern bands
- Quantum anomalous Hall crystal at fractional filling of moiré superlattices
- The Landau level: Half-full or half-empty?
- Spins, charges and currents at Domain Walls in a Quantum Hall Ising Ferromagnet
- Spontaneous Symmetry Breaking and Exotic Quantum Order in Integer Quantum Hall Systems under a Tilted Magnetic Field
- Magnetoplasmon Excitations and Spin Density Instabilities in an Integer Quantum Hall System with a Tilted Magnetic Field
- Condensation of Lattice Defects and Melting Transitions in Quantum Hall phases
- From Fractional Quantum Anomalous Hall Smectics to Polar Smectic Metals: Nontrivial Interplay Between Electronic Liquid Crystal Order and Topological Order in Correlated Topological Flat Bands
- Fractional Chern Insulator and Quantum Anomalous Hall Crystal in Twisted MoTe
- Designing (higher) Hall crystals
- Charge Density Wave-Assisted Tunneling Between Hall Edge States