Tuning the S=1/2 square-lattice antiferromagnet Sr2Cu(Te1-xWx)O6 from Neel order to quantum disorder to columnar order

被引:43
作者
Mustonen, O. [1 ]
Vasala, S. [2 ]
Schmidt, K. P. [3 ]
Sadrollahi, E. [3 ]
Walker, H. C. [4 ]
Terasaki, I. [5 ]
Litterst, F. J. [2 ,3 ]
Baggio-Saitovitch, E. [2 ]
Karppinen, M. [1 ]
机构
[1] Aalto Univ, Dept Chem & Mat Sci, FI-00076 Espoo, Finland
[2] CBPF, Rua Dr Xavier Sigaud 150, BR-22290180 Rio De Janeiro, Brazil
[3] Tech Univ Carolo Wilhelmina Braunschweig, Inst Phys Kondensierten Materie, D-38110 Braunschweig, Germany
[4] Rutherford Appleton Lab, ISIS Neutron & Muon Source, Didcot OX11 0QX, Oxon, England
[5] Nagoya Univ, Dept Phys, Nagoya, Aichi 4648602, Japan
关键词
HEISENBERG-ANTIFERROMAGNET; STATE; INSULATORS; CRYSTAL; MODEL; SR;
D O I
10.1103/PhysRevB.98.064411
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The spin-1/2 square-lattice Heisenberg model is predicted to have a quantum disordered ground state when magnetic frustration is maximized by competing nearest-neighbor J(1) and next-nearest-neighbor J(2) interactions (J(2)/J(1 )approximate to 0.5). The double perovskites Sr2CuTeO6 and Sr2CuWO6 are isostructural spin-1/2 square-lattice antiferromagnets with Neel (J(1) dominates) and columnar (J(2) dominates) magnetic order, respectively. Here we characterize the full isostructural solid solution series Sr2Cu(Te1-xWx)O-6 (0 <= x <= 1) tunable from Neel order to quantum disorder to columnar order. A spin-liquid-like ground state was previously observed for the x = 0.5 phase, but we show that the magnetic order is suppressed below 1.5 K in a much wider region of x approximate to 0.1-0.6. This coincides with significant T-linear terms in the low-temperature specific heat. However, density functional theory calculations predict most of the materials are not in the highly frustrated J(2)/J(1 )approximate to 0.5 region square-lattice Heisenberg model. Thus, a combination of both magnetic frustration and quenched disorder is the likely origin of the spin-liquid-like state in x = 0.5.
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页数:9
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