English

Successive phase transitions and quantum magnetization plateau in the spin-1 triangular-lattice antiferromagnet Ba$_2$La$_2$NiTe$_2$O$_{12}$

Strongly Correlated Electrons 2019-08-28 v2

Abstract

The crystal structure and magnetic properties of the spin-1 triangular-lattice antiferromagnet Ba2_2La2_2NiTe2_2O12_{12} are reported. Its crystal structure is trigonal R3ˉR\bar{3}, which is the same as that of Ba2_2La2_2NiW2_2O12_{12} [Y. Doi et al., J. Phys.: Condens. Matter 29, 365802 (2017)]. However, the exchange interaction J/kB19J/k_{\mathrm{B}}\simeq19 K is much greater than that observed in the tungsten system. At zero magnetic field, Ba2_2La2_2NiTe2_2O12_{12} undergoes successive magnetic phase transitions at TN1=9.8T_{\mathrm{N}1}=9.8 K and TN2=8.9T_{\mathrm{N}2}=8.9 K. The ground state is accompanied by a weak ferromagnetic moment. These results indicate that the ground-state spin structure is a triangular structure in a plane perpendicular to the triangular lattice owing to the small easy-axis-type anisotropy. The magnetization curve exhibits the one-third plateau characteristic of a two-dimensional triangular-lattice Heisenberg-like antiferromagnet. Exchange constants are also evaluated using density functional theory (DFT). The DFT results demonstrate the large difference in the exchange constants between tellurium and tungsten systems and the good two-dimensionality of the tellurium system.

Keywords

Cite

@article{arxiv.1903.08417,
  title  = {Successive phase transitions and quantum magnetization plateau in the spin-1 triangular-lattice antiferromagnet Ba$_2$La$_2$NiTe$_2$O$_{12}$},
  author = {Mutsuki Saito and Masari Watanabe and Nobuyuki Kurita and Akira Matsuo and Koichi Kindo and Maxim Avdeev and Harald O. Jeschke and Hidekazu Tanaka},
  journal= {arXiv preprint arXiv:1903.08417},
  year   = {2019}
}

Comments

12 pages, 15 figures, 4 tables