Quantum Hall Ferromagnetism in Graphene
Kentaro Nomura, A. H. MacDonald
Abstract
Graphene is a two-dimensional carbon material with a honeycomb lattice and Dirac-like low-energy excitations. When Zeeman and spin-orbit interactions are neglected its Landau levels are four-fold degenerate, explaining the 4 e2/h separation between quantized Hall conductivity values seen in recent experiments. In this paper we derive a criterion for the occurrence of interaction-driven quantum Hall effects near intermediate integer values of e2/h due to charge gaps in broken symmetry states.
Create a lesson
Related papers
ConvexAD: differentiable phase retrieval with geometric regularization for high-strain, low-signal Bragg coherent diffraction imaging
Matteo Masto, Ewen Bellec, Etienne Polack et al.
Symmetry-protected isolation of the quantum metric in chiral type-II semi-Dirac semimetals
Wen-Hao Bian, Jing Wang
Torsion, valley holonomy, and Berry phases of quasiparticles encircling dislocations and defect complexes in graphene
G. Q. Garcia, A. M. de M. Carvalho, C. Furtado
Field-free transverse response in altermagnet and topological insulator heterojunctions
Bijay Kumar Sahoo, Abhiram Soori
Nonlinearity-Induced Suppression of Dissipation in Bath-Coupled Floquet Topological Insulators
Bhoomija Chaurasia, Sebabrata Mukherjee
Dissipationless valley diode effects in Kekulé graphene superlattices
W. Zeng