Confinement-driven electronic and topological phases in corundum-derived $3d$-oxide honeycomb lattices

Abstract

Using density functional theory calculations including an on-site Coulomb term, we explore electronic and possibly topologically nontrivial phases in $3d$ transition metal oxide honeycomb layers confined in the corundum structure ($\alpha$-Al${}_2$O${}_3$) along the [0001] direction. In most cases the ground state is a trivial antiferromagnetic Mott insulator, often with distinct orbital or spin states compared to the bulk phases. With imposed symmetry of the two sublattices the ferromagnetic phases of Ti, Mn, Co and Ni exhibit a characteristic set of four bands, two relatively flat and two with a Dirac crossing at K, associated with the single electron occupation of $e_g^{\prime }$ (Ti) or $e_g$ (Mn, Co, Ni) orbitals. Our results indicate that the Dirac point can be tuned to the Fermi level using strain. Applying spin-orbit coupling (SOC) leads to a substantial anomalous Hall conductivity with values up to 0.94 $e^2/h$. Moreover, at $a_{A{l}_2{O}_3}$=4.81Å we identify a particularly strong effect of SOC with out-of-plane easy axis for ($T{i}_2$O${}_3$)${}_1$/(Al${}_2$O${}_3$)${}_5$(0001) which stabilizes dynamically the system. Due to the unusually high orbital moment of -0.88${\mu }_{\mathrm{B}}$ that nearly compensates the spin moment of 1.01${\mu }_{\mathrm{B}}$, this system emerges as a candidate for the realization of the topological Haldane model of spinless fermions. Parallels to the perovskite analogs (La$X$O${}_3$)${}_2$/(LaAlO${}_3$)${}_4$(111) are discussed.

arXiv comment9 pages, 9 figures

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