Abstract

Based on density functional theory calculations including a Coulomb repulsion parameter U, we explore the topological properties of (LaXO3)2/(LaAlO3)4 (111) with X = 4d and 5d cations. The metastable ferromagnetic phases of LaTcO3 and LaPtO3 with preserved P321 symmetry emerge as Chern insulators (CI) with C = 2 and 1 and band gaps of 41 and 38 meV at the lateral lattice constant of LaAlO3, respectively. Berry curvatures, spin textures as well as edge states provide additional insight into the nature of the CI states. While for X = Tc the CI phase is further stabilized under tensile strain, for X = Pd and Pt a site disproportionation takes place when increasing the lateral lattice constant from aLAO to aLNO. The CI phase of X = Pt shows a strong dependence on the Hubbard U parameter with sign reversal for higher values associated with the change of band gap opening mechanism. Parallels to the previously studied (X2O3)1/(Al2O3)5 (0001) honeycomb corundum layers are discussed. Additionally, non-magnetic systems with X = Mo and W are identified as potential candidates for Z2 topological insulators at aLAO with band gaps of 26 and 60 meV, respectively. The computed edge states and Z2 invariants underpin the non-trivial topological properties.

Highlights

  • The metastable ferromagnetic phases of LaTcO3 and LaPtO3 with preserved P321 symmetry emerge as Chern insulators (CI) with C = 2 and 1 and band gaps of 41 and 38 meV at the lateral lattice constant of LaAlO3, respectively

  • Our previous study[33] on corundum-derived superlattices with honeycomb pattern and X = 4d or 5d ion showed that the metastable ferromagnetic cases of X = Tc, Pt host quantum anomalous Hall states

  • Since at aLNO both LaPdO3 and LaPtO3 result in trivial Mott insulators due to site disproportionation, we explore here the topological properties at aLAO, where the P321 symmetry is preserved

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Summary

Introduction

The metastable ferromagnetic phases of LaTcO3 and LaPtO3 with preserved P321 symmetry emerge as Chern insulators (CI) with C = 2 and 1 and band gaps of 41 and 38 meV at the lateral lattice constant of LaAlO3, respectively. The ground states of X = Tc, Pd and Pt in (LaXO3)2/(LaAlO3)[4] (111) superlattices are AFM, (cf Table 1) with symmetry lowering due to a dimerization, manifested in alternating X–X bond lengths (not shown here), we concentrate here on the metastable ferromagnetic phases and explore their topological properties.

Results
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