Quantum-metric-induced quantum Hall conductance inversion and reentrant transition in fractional Chern insulators
arXiv:2407.07894 · doi:10.1103/PhysRevResearch.6.L032063
Abstract
The quantum metric of single-particle wave functions in topological flatbands plays a crucial role in determining the stability of fractional Chern insulating (FCI) states. Here, we unravel that the quantum metric causes the many-body Chern number of the FCI states to deviate sharply from the expected value associated with partial filling of the single-particle topological flatband. Furthermore, the variation of the quantum metric in momentum space induces band dispersion through interactions, affecting the stability of the FCI states. This causes a reentrant transition into the Fermi liquid from the FCI phase as the interaction strength increases.
18 pages, 10 figures
References in corpus (10)
- High temperature fractional quantum Hall states
- Fractional quantum Hall states at zero magnetic field
- Nearly-flat bands with nontrivial topology
- Signatures of Fractional Quantum Anomalous Hall States in Twisted MoTe2 Bilayer
- Observation of Fractionally Quantized Anomalous Hall Effect
- Fractional quantum Hall effect in the absence of Landau levels
- Quantum metric nonlinear Hall effect in a topological antiferromagnetic heterostructure
- Fluctuations, uncertainty relations, and the geometry of quantum state manifolds
- Engineering geometrically flat Chern bands with Fubini-Study Kähler structure
- Trial wave functions for a Composite Fermi liquid on a torus