4.6 Article

Topological Classification of Correlations in 2D Electron Systems in Magnetic or Berry Fields

Journal

MATERIALS
Volume 14, Issue 7, Pages -

Publisher

MDPI
DOI: 10.3390/ma14071650

Keywords

homotopy phases; long-range quantum entanglement; FQHE; Hall systems; Chern topological insulators

Funding

  1. Polish National Science Center [P.2016/21/D/ST3/00958]

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The recent research focuses on the classification of 2D electron states induced by different mappings of the planar Brillouin zone, as well as the classification of various phases of multi-electron homotopy patterns induced by Coulomb interaction. The presence of long-range quantum entanglement is essential for homotopy correlated phases, which are topologically protected and immune to local crystal field and disorder. The classification of homotopy long-range correlated phases is based on homotopy invariants and has been demonstrated through experimental observations in various materials.
Recent topology classification of 2D electron states induced by different homotopy classes of mappings of the planar Brillouin zone into Bloch space can be supplemented by a homotopy classification of various phases of multi-electron homotopy patterns induced by Coulomb interaction between electrons. The general classification of such type is presented. It explains the topologically protected correlations responsible for integer and fractional Hall effects in 2D multi-electron systems in the presence of perpendicular quantizing magnetic field or Berry field, the latter in topological Chern insulators. The long-range quantum entanglement is essential for homotopy correlated phases in contrast to local binary entanglement for conventional phases with local order parameters. The classification of homotopy long-range correlated phases induced by the Coulomb interaction of electrons has been derived in terms of homotopy invariants and illustrated by experimental observations in GaAs 2DES, graphene monolayer, and bilayer and in Chern topological insulators. The homotopy phases are demonstrated to be topologically protected and immune to the local crystal field, local disorder, and variation of the electron interaction strength. The nonzero interaction between electrons is shown, however, to be essential for the definition of the homotopy invariants, which disappear in gaseous systems.

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