Bond directional anapole state in a spin-orbit coupled Mott insulator Sr<sub>2</sub>(Ir<sub>1−x</sub>Rh<sub>x</sub>)O<sub>4</sub>
ORAL
Abstract
In a spin-orbit coupled Mott insulator Sr2(Ir1−xRhx)O4, a possible hidden order phase has been reported distinctly above the Néel order phase, accompanying both inversion and time-reversal symmetry breakings. However, the nature of this mysterious phase remains largely elusive. We provide a detailed study of the hidden order phase through the combined study of in-plane magnetic torque and the nematic susceptibility measurements [1]. Our torque magnetometry provides thermodynamic evidence for an electronic nematic transition, breaking C4 rotational symmetry of the underlying lattice. However, in contrast to ordinal even-parity nematic orders, the nematic susceptibility exhibits no divergent behavior towards the onset of the hidden order. These results imply that the nematicity is not a primary order parameter but a secondary one of an odd-parity order parameter. Moreover, our results demonstrate that the hidden order phase is consistent with a bond directional anapole order, in which the intra-unit-cell loop current flows along only one of the diagonal directions in the IrO4 square.
[1] H. Murayama, et al., arXiv:2008.06380.
[1] H. Murayama, et al., arXiv:2008.06380.
*This work is supported by KAKENHI, Innovative Areas “Quantum Liquid Crystals” from JSPS, and JST CREST. GC acknowledges NFS support via grant DMR 1903888.
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Presenters
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Hinako Murayama
- Department of physics, Kyoto University