Ordered magnetic phases of the frustrated spin-dimer compound Ba3Mn2O8

被引:41
|
作者
Samulon, E. C. [1 ,2 ]
Jo, Y. -J. [3 ]
Sengupta, P. [4 ,5 ]
Batista, C. D. [4 ]
Jaime, M. [5 ]
Balicas, L. [3 ]
Fisher, I. R. [1 ,2 ]
机构
[1] Stanford Univ, Geballe Lab Adv Mat, Stanford, CA 94305 USA
[2] Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
[3] Florida State Univ, Natl High Magnet Field Lab, Tallahassee, FL 32306 USA
[4] Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545 USA
[5] Los Alamos Natl Lab, Nat High Magnet Field Lab, Los Alamos, NM 87545 USA
来源
PHYSICAL REVIEW B | 2008年 / 77卷 / 21期
关键词
D O I
10.1103/PhysRevB.77.214441
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Ba(3)Mn(2)O(8) is a spin-dimer compound based on pairs of S=1, 3d(2), Mn(5+) ions arranged on a triangular lattice. Antiferromagnetic intradimer exchange leads to a singlet ground state in zero field. Here we present the first results of thermodynamic measurements for single crystals probing the high-field ordered states of this material associated with closing the spin gap to the excited triplet states. Specific heat, magnetocaloric effect, and torque magnetometry measurements were performed in magnetic fields up to 32 T and temperatures down to 20 mK. For fields above H(c1)similar to 8.7 T, these measurements reveal a single magnetic phase for H parallel to c but two distinct phases (approximately symmetric about the center of the phase diagram) for H perpendicular to c. Analysis of the simplest possible spin Hamiltonian describing this system yields candidates for these ordered states corresponding to a simple spiral structure for H parallel to c and to two distinct modulated phases for H perpendicular to c. Both single-ion anisotropy and geometric frustration play crucial roles in defining the phase diagram.
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页数:13
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