NaCuMoO_4(OH) as a Candidate Frustrated J_1-J_2 Chain Quantum Magnet
arXiv:1409.1310 · doi:10.7566/JPSJ.83.103702
Abstract
In a frustrated J_1-J_2 chain with the nearest-neighbor ferromagnetic interaction J_1 and the next-nearest-neighbor antiferromagnetic interaction J_2, novel magnetic states such as a spin-nematic state are theoretically expected. However, they have been rarely examined in experiments because of the difficulty in obtaining suitable model compounds. We show here that the quasi-one-dimensional antiferromagnet NaCuMoO_4(OH), which comprises edge-sharing CuO_2 chains, is a good candidate J_1-J_2 chain antiferromagnet. The exchange interactions are estimated as J_1 = - 51 K and J_2 = 36 K by comparing the magnetic susceptibility, heat capacity, and magnetization data with the data obtained using calculations by the exact diagonalization method. High-field magnetization measurements at 1.3 K show a saturation above 26 T with little evidence of a spin nematic state expected just below the saturation field, which is probably due to smearing effects caused by thermal fluctuations and the polycrystalline nature of the sample.
6 pages, 4 figures
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- The dynamics of linarite: Observations of magnetic excitations
- Bose-Einstein condensation of a two-magnon bound state in a spin-one triangular lattice
- Orbital Arrangements and Magnetic Interactions in the Quasi-One-Dimensional Cuprates ACuMoO_4(OH) (A = Na, K)
- Angular dependence of electron spin resonance for detecting quadrupolar liquid state of frustrated spin chains
- The magnetic phase diagram of the frustrated spin chain compound linarite, PbCuSO(OH), as seen by neutron diffraction and H-NMR
- Collinear Spin-density-wave Order and Anisotropic Spin Fluctuations in the Frustrated -- Chain Magnet NaCuMoO(OH)
- Highly dispersive magnons with spin-gap like features in the frustrated ferromagnetic S=1/2 chain compound Ca2Y2Cu5O10 detected by inelastic neutron scattering
- Control of superexchange interactions with DC electric fields
- Anisotropic Field-Induced Gap in Quasi-One-Dimensional Antiferromagnet KCuMoO(OH)
- Pressure-induced phase transition in the - square lattice antiferromagnet RbMoOPOCl