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Lattice distortion effects on the frustrated spin-1 triangular-antiferromagnet A_3NiNb_2O_9 (A = Ba, Sr, and Ca)

机译:晶格畸变对受挫的spin-1三角反磁体A_3NiNb_2O_9(A = Ba,Sr和Ca)的影响

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摘要

In geometrically frustrated materials with low-dimensional and small spin moment, the quantum fluctuation can interfere with the complicated interplay of the spin, electron, lattice, and orbital interactions, and host exotic ground states such as the nematic spin state and chiral liquid phase. While the quantum phases of the one-dimensional chain and S = 1/2 two-dimensional triangular-lattice antiferromagnet (TLAF) have been more thoroughly investigated by both theorists and experimentalists, the work on the 5 = 1 TLAF has been limited. We induced the lattice distortion into the TLAFs A_3NiNb_2O_9 (A = Ba, Sr, and Ca) with S(Ni~(2+)) = 1, and applied thermodynamic, magnetic, and neutron scattering measurements. Although A_3NiNb_2O_9 kept the noncollinear 120° antiferromagnetic phase as the ground state, the Ni~(2+) lattice changed from an equilateral triangle (A = Ba) into an isosceles triangle (A = Sr and Ca). The inelastic neutron scattering data were simulated by the linear spin-wave theory, and the competition between the single-ion anisotropy and the exchange anisotropy from the distorted lattice are discussed.
机译:在具有低维和小自旋矩的几何受阻材料中,量子涨落会干扰自旋,电子,晶格和轨道相互作用的复杂相互作用,并拥有诸如向列自旋态和手性液相等奇异的基态。虽然理论家和实验家都对一维链和S = 1/2二维三角晶格反铁磁体(TLAF)的量子相进行了更彻底的研究,但对5 = 1 TLAF的研究却受到了限制。我们在S(Ni〜(2+))= 1的情况下,将晶格畸变引入TLAF A_3NiNb_2O_9(A = Ba,Sr和Ca)中,并进行了热力学,磁和中子散射测量。尽管A_3NiNb_2O_9保持非共线120°反铁磁相为基态,但Ni〜(2+)晶格从等边三角形(A = Ba)变为等腰三角形(A = Sr和Ca)。利用线性自旋波理论模拟了非弹性中子散射数据,并讨论了畸变晶格中单离子各向异性与交换各向异性之间的竞争。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第9期|094412.1-094412.10|共10页
  • 作者单位

    Helmholtz-Zentrum Berlin fuer Materialien und Energie, D-14109 Berlin, Germany;

    School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332, USA;

    Key Laboratory of Artificial Structures and Quantum Control, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China;

    Helmholtz-Zentrum Berlin fuer Materialien und Energie, D-14109 Berlin, Germany;

    Helmholtz-Zentrum Berlin fuer Materialien und Energie, D-14109 Berlin, Germany;

    Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA;

    Key Laboratory of Artificial Structures and Quantum Control, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China,Collaborative Innovation Center of Advanced Microstructures, Nanjing, Jiangsu 210093, China;

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