Topological origin of flat-bands as pseudo-Landau levels in uniaxial strained graphene nanoribbons and induced magnetic ordering due to electron-electron interactions
arXiv:2303.04262 · doi:10.1103/PhysRevB.107.235143
Abstract
Flat-bands play a central role in the presence of correlated phases in Moiré and other modulated two dimensional systems. In this work, flat-bands are shown to exist in uniaxially periodic strained graphene. Such strain should be produced for example by a substrate. The model is thus mapped into a one-dimensional effective Hamiltonian and this allows to find the conditions for having flat-bands, i.e., a long-wavelength modulation only on each one of the bipartite graphene sublattices, while having a tagged strain field between neighboring carbon atoms. The origin of such flat-bands is thus tracked down to the existence of topological localized wavefunctions at domain walls separating different regions, each with a non-uniform Su-Schriffer-Hegger model (SSH) type of coupling. Thereafter, the system is mapped into a continuum model allowing to explain the numerical results in terms of the Jackiw-Rebbi model and of pseudo-Landau levels. Finally, the interplay between the obtained flat-bands and electron-electron interaction is explored through the Hubbard model. The numerical results within the mean-field approximation indicate that the flat-bands induce Néel antiferromagnetic and ferromagnetic domains even for a very weak Hubbard interaction. The present model thus provides a simple platform to understand the physical origin of flat-bands, pseudo-Landau levels and the effects of the electron-electron interaction.
10 pages, 9 figures
References in corpus (19)
- Tunable Phase Boundaries and Ultra-Strong Coupling Superconductivity in Mirror Symmetric Magic-Angle Trilayer Graphene
- Continuum Model of the Twisted Bilayer
- Nematicity and Competing Orders in Superconducting Magic-Angle Graphene
- Absence of a Spin Liquid Phase in the Hubbard Model on the Honeycomb Lattice
- Charge-polarized interfacial superlattices in marginally twisted hexagonal boron nitride
- Exotic electronic states in the world of flat bands: from theory to material
- Evidence of Flat Bands and Correlated States in Buckled Graphene Superlattices
- Continuum models for twisted bilayer graphene: the effects of lattice deformation and hopping parameter
- Tuning the pseudospin polarization of graphene by a pseudo-magnetic field
- Flat bands and perfect metal in trilayer moiré graphene
- The Hubbard model on the honeycomb lattice: from static and dynamical mean-field theories to lattice quantum Monte Carlo simulations
- Mapping of strained graphene into one-dimensional Hamiltonians: quasicrystals and modulated crystals
- Reduction of the Twisted Bilayer Graphene Chiral Hamiltonian into a matrix operator and physical origin of flat-bands at magic angles
- Topological flat bands in time-periodically driven uniaxial strained graphene nanoribbons
- Topological edge states on time-periodically strained armchair graphene nanoribbons
- Dirac-Harper Theory for One Dimensional Moiré Superlattices
- Origami-controlled strain engineering of tunable flat bands and correlated states in folded graphene
- Analytic solution to pseudo-Landau levels in strongly bent graphene nanoribbons
- Exact Diagonalization Study of 2D Hubbard Model on Honeycomb Lattice: Semi-metal-Insulator Transition
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- Finite temperatures and flat bands: the Hubbard model on three-dimensional Lieb lattices
- Protected Fermionic Zero Modes in Periodic Gauge Fields
- Designing Flat Bands and Pseudo-Landau Levels in GaAs with Patterned Gates
- Interaction-driven charge textures and unconventional superconductivity in strained monolayer graphene
- Dislocation Patterning as a Mechanism for Flat Band Formation