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Quantum spin Hall insulator on the honeycomb lattice induced by ferromagnetic exchange interaction
We study the many-body instabilities of correlated electrons on the half-filled honeycomb lattice with enhanced exchange coupling. The system is described by an extended Hubbard model including the next-nearest-neighbor Coulomb repulsion (\(V_2\)) and the nearest-neighbor exchange interaction (\(J\)...
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creator | Ye-Un An Song-Jin, O Kwang-Il Ryom Il-Gwang Son |
description | We study the many-body instabilities of correlated electrons on the half-filled honeycomb lattice with enhanced exchange coupling. The system is described by an extended Hubbard model including the next-nearest-neighbor Coulomb repulsion (\(V_2\)) and the nearest-neighbor exchange interaction (\(J\)). We use the truncated unity functional renormalization group approach to determine a schematic ground-state phase diagram with higher resolution in the parameter space of \(V_2\) and \(J\). In the absence of the on-site repulsion and presence of sizable next-nearest-neighbor repulsion and enhanced nearest-neighbor exchange interaction, we encounter the quantum spin Hall phase, the spin-Kekul\'{e} phase, and the three-sublattice and the incommensurate charge-density-wave phases. We propose a scheme for combining consistently the truncated unity functional renormalization group and the mean-field approximation, which is distinct from the conventional one that directly uses the renormalization-group results as an input for the mean-field calculation. This scheme is used to study in detail the quantum spin Hall phase, presenting some characteristics like the bulk gap, the Chern number and the helical edge states. |
doi_str_mv | 10.48550/arxiv.2301.09838 |
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The system is described by an extended Hubbard model including the next-nearest-neighbor Coulomb repulsion (\(V_2\)) and the nearest-neighbor exchange interaction (\(J\)). We use the truncated unity functional renormalization group approach to determine a schematic ground-state phase diagram with higher resolution in the parameter space of \(V_2\) and \(J\). In the absence of the on-site repulsion and presence of sizable next-nearest-neighbor repulsion and enhanced nearest-neighbor exchange interaction, we encounter the quantum spin Hall phase, the spin-Kekul\'{e} phase, and the three-sublattice and the incommensurate charge-density-wave phases. We propose a scheme for combining consistently the truncated unity functional renormalization group and the mean-field approximation, which is distinct from the conventional one that directly uses the renormalization-group results as an input for the mean-field calculation. 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subjects | Charge density waves Exchanging Ferromagnetism Phase diagrams Unity |
title | Quantum spin Hall insulator on the honeycomb lattice induced by ferromagnetic exchange interaction |
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