Electron and hole doping in the relativistic Mott insulator SrIrO: a first-principles study using band unfolding technique
arXiv:1606.09112 · doi:10.1103/PhysRevB.94.195145
Abstract
We study the effects of dilute La and Rh doping on the electronic structure of the relativistic Mott insulator SrIrO using fully relativistic and magnetically non-collinear density functional theory with the inclusion of an on-site Hubbard . To model doping effects, we have adopted the supercell approach that allows for a realistic treatment of structural relaxations and electronic effects beyond a purely rigid band approach. By means of the band unfolding technique we have computed the spectral function and constructed the effective band structure and Fermi surface (FS), which are readily comparable with available experimental data. Our calculations clearly indicate that La and Rh doping can be interpreted as effective electron and (fractional) hole doping, respectively. In SrLaIrO the IMT is accompanied by a moderate renormalization of the electronic correlation substantiated by a reduction of the effective on-site Coulomb repulsion from 1.6 eV () to 1.4 eV (metallic regime ). The progressive closing of the relativistic Mott gap leads to the emergence of connected elliptical electron pockets at (/2,/2) and less intense features at in the FS. The substitution of Ir with the nominally isovalent Rh is accompanied by a substantial hole transfer from the Rh site to the nearest neighbor Ir sites. This shifts down the chemical potential, creates almost circular disconnected hole pockets in the FS and establishes the emergence of a two-dimensional metallic state formed by conducting Rh-planes intercalated by insulating Ir-planes. Finally, our data indicate that hole doping causes a flipping of the in-plane net ferromagnetic moment in the Rh plane and induces a magnetic transition from the AF-I to the AF-II ordering.
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- Doping-induced insulator-metal transition in the Lifshitz magnetic insulator NaOsO3
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- The "dark phase'' in SrIrRhO revealed by Seebeck and Hall measurements