<p>We use magnetization measurements under pressure along with ab initio and cluster many-body calculations to investigate magnetism of the Kitaev candidate Li<sub>2</sub>RhO<sub>3</sub>. Hydrostatic compression leads to a decrease in the magnitude of the nearest-neighbor ferromagnetic Kitaev coupling <i>K</i><sub>1</sub> and the corresponding increase in the off-diagonal anisotropy Γ<sub>1</sub>, whereas the experimental Curie-Weiss temperature changes from negative to positive with the slope of +40 K/GPa. On the other hand, spin freezing persists up to at least 3.46 GPa with the almost constant freezing temperature of 5 K that does not follow the large changes in the exchange couplings and indicates the likely extrinsic origin of spin freezing. Magnetic frustration in Li<sub>2</sub>RhO<sub>3</sub> is mainly related to the interplay between ferromagnetic <i>K</i><sub>1</sub> and antiferromagnetic Γ<sub>1</sub>, along with the weakness of the third-neighbor coupling <i>J</i><sub>3</sub> that would otherwise stabilize zigzag order. The small <i>J</i><sub>3</sub> distinguishes Li<sub>2</sub>RhO<sub>3</sub> from other Kitaev candidates.</p>

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Pressure-dependent magnetism of the Kitaev candidate Li2RhO3

  • Bin Shen,
  • Efrain Insuasti Pazmino,
  • Ramesh Dhakal,
  • Friedrich Freund,
  • Philipp Gegenwart,
  • Stephen M. Winter,
  • Alexander A. Tsirlin

摘要

We use magnetization measurements under pressure along with ab initio and cluster many-body calculations to investigate magnetism of the Kitaev candidate Li2RhO3. Hydrostatic compression leads to a decrease in the magnitude of the nearest-neighbor ferromagnetic Kitaev coupling K1 and the corresponding increase in the off-diagonal anisotropy Γ1, whereas the experimental Curie-Weiss temperature changes from negative to positive with the slope of +40 K/GPa. On the other hand, spin freezing persists up to at least 3.46 GPa with the almost constant freezing temperature of 5 K that does not follow the large changes in the exchange couplings and indicates the likely extrinsic origin of spin freezing. Magnetic frustration in Li2RhO3 is mainly related to the interplay between ferromagnetic K1 and antiferromagnetic Γ1, along with the weakness of the third-neighbor coupling J3 that would otherwise stabilize zigzag order. The small J3 distinguishes Li2RhO3 from other Kitaev candidates.