Optical anisotropy of the Jeff = 1/2 Mott insulator Sr2IrO4
D. Pr\"opper, A. N. Yaresko, M. H\"oppner, Y. Matiks, Y.-L. Mathis, T., Takayama, A. Matsumoto, H. Takagi, B. Keimer, A. V. Boris

TL;DR
This study investigates the optical anisotropy of Sr2IrO4, revealing strong directional dependence in its dielectric response due to electronic transitions between specific iridium bands, supported by experimental and theoretical analysis.
Contribution
It provides detailed measurements of the dielectric function along different crystallographic axes and compares them with first-principle calculations, highlighting anisotropic optical properties in a Jeff=1/2 Mott insulator.
Findings
Identified 10 infrared-active phonon modes in-plane and 4 along c-axis.
Observed strong optical anisotropy in near-infrared spectra.
Transition probabilities between Ir 5d bands are highly polarization-dependent.
Abstract
We report the complex dielectric function along and perpendicular to the IrO2 planes in the layered perovskite Sr2IrO4 determined by spectroscopic ellipsometry in the spectral range from 12 meV to 6 eV. Thin high quality single crystals were stacked to measure the c-axis optical conductivity. In the phonon response we identified 10 infrared-active modes polarized within the basal plane and only four modes polarized along the c-axis, in full agreement with first-principle lattice dynamics calculations. We also observed a strong optical anisotropy in the near-infrared spectra arising from direct transitions between Ir 5d t2g Jeff = 1/2 and Jeff = 3/2 bands, which transition probability is highly suppressed for light polarized along the c-axis. The spectra are analyzed and discussed in terms of relativistic LSDA+U band structure calculations.
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
