Spin-liquid-like state in a spin-1/2 square-lattice antiferromagnet perovskite induced by d<sup>10</sup>-d<sup>0</sup> cation mixing.

Mustonen, O; Vasala, S; Sadrollahi, E; Schmidt, K P; Baines, C; Walker, H C; Terasaki, I; Litterst, F J et al. · Nat Commun · 2018

basic_science · Level V

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Abstract

A quantum spin liquid state has long been predicted to arise in spin-1/2 Heisenberg square-lattice antiferromagnets at the boundary region between Néel (nearest-neighbor interaction dominates) and columnar (next-nearest-neighbor interaction dominates) antiferromagnetic order. However, there are no known compounds in this region. Here we use d<sup>10</sup>-d<sup>0</sup> cation mixing to tune the magnetic interactions on the square lattice while simultaneously introducing disorder. We find spin-liquid-like behavior in the double perovskite Sr<sub>2</sub>Cu(Te<sub>0.5</sub>W<sub>0.5</sub>)O<sub>6</sub>, where the isostructural end phases Sr<sub>2</sub>CuTeO<sub>6</sub> and Sr<sub>2</sub>CuWO<sub>6</sub> are Néel and columnar type antiferromagnets, respectively. We show that magnetism in Sr<sub>2</sub>Cu(Te<sub>0.5</sub>W<sub>0.5</sub>)O<sub>6</sub> is entirely dynamic down to 19 mK. Additionally, we observe at low temperatures for Sr<sub>2</sub>Cu(Te<sub>0.5</sub>W<sub>0.5</sub>)O<sub>6</sub>-similar to several spin liquid candidates-a plateau in muon spin relaxation rate and a strong T-linear dependence in specific heat. Our observations for Sr<sub>2</sub>Cu(Te<sub>0.5</sub>W<sub>0.5</sub>)O<sub>6</sub> highlight the role of disorder in addition to magnetic frustration in spin liquid physics.