Frustrated Heisenberg J1-J2 model within the stretched diamond lattice of LiYbO2

被引:0
作者
Bordelon, Mitchell M. [1 ]
Liu, Chunxiao [2 ]
Posthuma, Lorenzo [1 ]
Kenney, Eric [3 ]
Graf, M. J. [3 ]
Butch, N. P. [4 ]
Banerjee, Arnab [5 ,6 ]
Calder, Stuart [5 ]
Balents, Leon [7 ]
Wilson, Stephen D. [1 ]
机构
[1] Univ Calif Santa Barbara, Mat Dept, Santa Barbara, CA 93106 USA
[2] Univ Calif Santa Barbara, Dept Phys, Santa Barbara, CA 93106 USA
[3] Boston Coll, Dept Phys, Chestnut Hill, MA 02467 USA
[4] NIST, Ctr Neutron Res, Gaithersburg, MD 20899 USA
[5] Oak Ridge Natl Lab, Neutron Scattering Div, POB 2009, Oak Ridge, TN 37831 USA
[6] Purdue Univ, Purdue Quantum Sci & Engn Inst, W Lafayette, IN 47906 USA
[7] Univ Calif Santa Barbara, Kavli Inst Theoret Phys, Santa Barbara, CA 93106 USA
基金
美国国家科学基金会;
关键词
EFFECTIVE IONIC-RADII; MAGNETIC-PROPERTIES; SPIN-LIQUID; OXIDES; ANTIFERROMAGNET; ORDER; DISORDER; STATE; LN;
D O I
10.1103/PhysRevB.103.014420
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We investigate the magnetic properties of LiYbO2, containing a three-dimensionally frustrated, diamondlike lattice via neutron scattering, magnetization, and heat capacity measurements. The stretched diamond network of Yb3+ ions in LiYbO2 enters a long-range incommensurate, helical state with an ordering wave vector k = (0.384,+/- 0.384, 0) that "locks-in" to a commensurate k = (1/3,+/- 1/3, 0) phase under the application of a magnetic field. The spiral magnetic ground state of LiYbO2 can be understood in the framework of a Heisenberg J(1)-J(2) Hamiltonian on a stretched diamond lattice, where the propagation vector of the spiral is uniquely determined by the ratio of J(2)/vertical bar J(1 vertical bar). The pure Heisenberg model, however, fails to account for the relative phasing between the Yb moments on the two sites of the bipartite lattice, and this detail as well as the presence of an intermediate, partially disordered, magnetic state below 1 K suggests interactions beyond the classical Heisenberg description of this material.
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页数:16
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