Role of non-local correlations for spectral properties of Sr<sub>2</sub>IrO<sub>4</sub>
ORAL
Abstract
The spin-orbit Mott insulator Sr2IrO4 has raised tremendous interest recently due to striking similarities to high-Tc superconducting copper oxides both in the pure and in electron-doped compounds.
Here, we study the evolution of the spectral function of this 5d transition metal system as a function of doping by means of a combined ab-initio electronic structure and many-body quantum cluster approach. Thereby, important ingredients like spin-orbit coupling and distortions of the oxygen octahedra as well as Hubbard interactions and non-local charge fluctuations are taken into account. The spectral function of pure Sr2IrO4 is analyzed both in its high-temperature paramagnetic and in its low-temperature antiferromagnetic phase and the importance of non-local fluctuations is discussed. The spectra compare well with angular-resolved photoemission measurements and allow to study emerging changes under electron- and hole-doping. Special emphasis is placed on pseudogap features of the spectral function of electron-doped Sr2IrO4, which are found to be in good agreement with experiment.
Here, we study the evolution of the spectral function of this 5d transition metal system as a function of doping by means of a combined ab-initio electronic structure and many-body quantum cluster approach. Thereby, important ingredients like spin-orbit coupling and distortions of the oxygen octahedra as well as Hubbard interactions and non-local charge fluctuations are taken into account. The spectral function of pure Sr2IrO4 is analyzed both in its high-temperature paramagnetic and in its low-temperature antiferromagnetic phase and the importance of non-local fluctuations is discussed. The spectra compare well with angular-resolved photoemission measurements and allow to study emerging changes under electron- and hole-doping. Special emphasis is placed on pseudogap features of the spectral function of electron-doped Sr2IrO4, which are found to be in good agreement with experiment.
*This work was supported by a Consolidator Grant of the European Research Council (CorrelMat-617196), the French Agence Nationale de la Recherche (ANR-15-CE30-0009-01) and IDRIS/GENCI Orsay (t2017091393).
–
Presenters
-
Benjamin Lenz
- Centre de Physique Théorique (CPHT), Ecole Polytechnique