Classification of Topological Phase Transitions and van Hove Singularity Steering Mechanism in Graphene Superlattices
arXiv:2006.13946 · doi:10.1103/PhysRevLett.125.236805
Abstract
We study quantum phase transitions in graphene superlattices in external magnetic fields, where a framework is presented to classify multiflavor Dirac fermion critical points describing hopping tuned topological phase transitions of integer and fractional Hofstadter-Chern insulators. We argue and provide numerical support for the existence of transitions that can be explained by a nontrivial interplay of Chern bands and van Hove singularities near charge neutrality. This work provides a route to critical phenomena beyond conventional quantum Hall plateau transitions.
Published version
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- Unconventional Self-Similar Hofstadter Superconductivity from Repulsive Interactions
- Fractional Chern Insulators in Twisted Bilayer MoTe: A Composite Fermion Perspective
- Topological phases of the dimerized Hofstadter butterfly
- Symmetry indicators in commensurate magnetic flux
- Replica Higher-Order Topology of Hofstadter Butterflies in Twisted Bilayer Graphene
- Topological van Hove singularities at phase transitions in Weyl metals
- Tunable interface states between Floquet-Weyl semimetals
- Correlated phases and topological phase transition in twisted bilayer graphene at one quantum of magnetic flux
- Magnetic Bloch States at Integer Flux Quanta Induced by Super-moiré Potential in Graphene Aligned with Twisted Boron Nitride
- Electromagnetic response and emergent topological orders in transition metal dichalcogenide MoTe bilayers
- Quantum Fractality on the Surface of Topological Insulators
- Bloch and Bethe ansatze for the Harper model: A butterfly with a boundary
- Topological constraints on the electronic band structure of hexagonal lattice in a magnetic field
- Hofstadter Butterfly in Graphene
- Theory of Hofstadter Superconductors
- Critical magnetic flux for Weyl points in the three-dimensional Hofstadter model
- Localization phase diagram of the Hexagonal Lattice with irrational magnetic flux