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High antiferromagnetic transition temperature of the honeycomb compound SrRu2O6
被引:39
|作者:
Tian, W.
[1
]
Svoboda, C.
[2
]
Ochi, M.
[3
]
Matsuda, M.
[1
]
Cao, H. B.
[1
]
Cheng, J. -G.
[4
,5
]
Sales, B. C.
[6
]
Mandrus, D. G.
[6
,7
]
Arita, R.
[3
]
Trivedi, N.
[2
]
Yan, J. -Q.
[6
,7
]
机构:
[1] Oak Ridge Natl Lab, Quantum Condensed Matter Div, Oak Ridge, TN 37831 USA
[2] Ohio State Univ, Dept Phys, Columbus, OH 43210 USA
[3] RIKEN Ctr Emergent Matter Sci, Wako, Saitama 3510198, Japan
[4] Chinese Acad Sci, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
[5] Chinese Acad Sci, Inst Phys, Beijing 100190, Peoples R China
[6] Oak Ridge Natl Lab, Mat Sci & Technol Div, Oak Ridge, TN 37831 USA
[7] Univ Tennessee, Dept Mat Sci & Engn, Knoxville, TN 37996 USA
来源:
基金:
美国国家科学基金会;
关键词:
POLARIZATION ANALYSIS;
D O I:
10.1103/PhysRevB.92.100404
中图分类号:
T [工业技术];
学科分类号:
08 ;
摘要:
We study the high-temperature magnetic order in a quasi-two-dimensional honeycomb compound SrRu2O6 by measuring magnetization and neutron powder diffraction with both polarized and unpolarized neutrons. SrRu2O6 crystallizes into the hexagonal lead antimonate (PbSb2O6, space group P (3) over bar 1m) structure with layers of edge-sharing RuO6 octahedra separated by Sr2+ ions. SrRu2O6 is found to order at T-N = 565 K with Ru moments coupled antiferromagnetically both in plane and out of plane. The magnetic moment is 1.30(2) mu(B)/Ru at room temperature and is along the crystallographic c axis in the G-type magnetic structure. We perform density functional calculations with constrained random-phase approximation (RPA) to obtain the electronic structure and effective intra-and interorbital interaction parameters. The projected density of states shows strong hybridization between Ru 4d and O 2p. By downfolding to the target t(2g) bands we extract the effective magnetic Hamiltonian and perform Monte Carlo simulations to determine the transition temperature as a function of interand intraplane couplings. We find a weak interplane coupling, 3% of the strong intraplane coupling, permits three-dimensional magnetic order at the observed T-N.
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