三角形晶格上自旋-1 \(J_{1} - J_{2}\)反铁磁海森堡模型的\(120^{0}\)有序相

V. H. Nguyen, T. N. Pham Thi, Thang Nguyen Toan
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引用次数: 0

摘要

在具有最近J1和次近邻J2交换作用的三角形晶格上,研究了量子涨落和热涨落对自旋-1反铁磁海森堡模型1200有序相的激发能谱和亚晶格磁化的影响。利用虚拉格朗日乘子的泛函积分形式中自旋算子的辅助费米子表示来保持单粒子占用的精确约束。用Luttinger-Tisza序向量Q表示经典基态时,可以考虑整个耦合参数范围内系统自由能的涨落贡献。我们推导了单回路近似的磁振子谱和考虑热波动的磁化强度。所得结果与线性自旋波近似的结果和化合物NiGa2S4的实验结果进行了比较。
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The \(120^{0}\) ordered phase of the spin-1 \(J_{1} - J_{2}\) antiferromagnetic Heisenbeberg model on a triangular lattice
We study the effect of quantum and thermal fluctuations on the excitation energy spectrum and sublattice magnetization of the 1200 ordered phase of the spin-1 antiferromagnetic Heisenberg model on a triangular lattice with nearest J1 and next-nearest-neighbor J2 exchange interactions. The auxiliary fermionic representation of the spin operators within a functional integral formalism with an imaginary Lagrange multiplier is employed to retain an exact constraint of single particle occupancy. Representing the classical ground state by Luttinger-Tisza ordering vector Q one may consider the fluctuation contributions to the free energy of the system in the entire range of the coupling parameters. We derived the magnon spectrum in one-loop approximation and the magnetization taking into account thermal fluctuations. The obtained results are compared with the result of the linear spin-wave approximation and experimental findings on compound NiGa2S4.
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