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arXiv:2209.04336 · Journal of Superconductivity and Novel Magnetism

Topological States in Strongly Correlated Systems

V. Yu. Irkhin, Yu. N. Skryabin

Published May 2, 2022• 5 citations
arXivHTMLPDF
DOI
10.1007/s10948-022-06251-3

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Abstract This paper considers modern ideas about the topological nature of superconductivity and the Mott–Hubbard state in strongly correlated systems. These systems are described in terms of spin and charge separation, i.e., deconfinement of spinons and holons in a gauge field. The role of orbital degrees of freedom is discussed. Analogies with topological insulators, quantum Hall effect, and Landau quantization are considered. The importance of the Chern–Simons term for the correct description of the Hubbard splitting is demonstrated.
Chiral topological orders formed in correlated fermion systems have been widely explored. However, the mechanism of how they emerge from interacting fermions is still unclear. Here, we propose a susceptibility condition. Under this condition, we show that chiral topological orders can spontaneously take place in correlated fermion systems. The condition leads to a low-energy effective theory of bosons with strong frustration, mimicking flat-band systems. The frustration then melts the long-range orders and results in topological orders with time-reversal symmetry breaking. We apply the theory to strongly correlated semiconductors doped to the metallic phase. An excitonic topological order with semionic excitations and a chiral excitonic edge state is revealed. We also discuss the application to frustrated magnets. The theory predicts a chiral spin-liquid state, which is numerically confirmed by our tensor network calculations. These results demonstrate an indicator for chiral topological orders, which bridges the existing gap between interacting fermions and correlated topological matter.