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Classical spin liquid properties of the infinite-component spin vector model on a fully frustrated two dimensional lattice

机译:完全挫折二维晶格上无限分量自旋矢量模型的经典自旋液体性质

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摘要

Thermodynamic quantities and correlation functions (CFs) of the classical antiferromagnet on the checkerboard lattice are studied for the exactly solvable infinite-component spin-vector model, D → ∞. In contrast to conventional two-dimensional magnets with continuous symmetry showing extended short-range order at distances smaller than the correlation length, r approx.< ξ_c ∝ exp(T~*/T), correlations in the checkerboard-lattice model decay already at the scale of the lattice spacing due to the strong degeneracy of the ground state characterized by a macroscopic number of strongly fluctuating local degrees of freedom. At low temperatures, spin CFs decay as ∝ 1/r~2 in the range a_0 r ξ_c ∝ T~(-1/2), where a_0 is the lattice spacing. Analytical results for the principal thermodynamic quantities in our model are very similar with MC simulations, exact and analytical results for the classical Heisenberg model (D = 3) on the pyrochlore lattice. This shows that the ground state of the infinite-component spin vector model on the checkerboard lattice is a classical spin liquid.
机译:针对可求解的无限分量自旋矢量模型D→∞,研究了经典反铁磁体在棋盘格上的热力学量和相关函数(CF)。与传统的具有连续对称性的二维磁体在距离小于相关长度r约<ξ_c∝ exp(T〜* / T)的距离处显示短距离有序扩展相比,棋盘格模型的相关性已经在晶格间距的尺度是由于基态的强烈退化而引起的,其特征在于宏观数量的剧烈波动的局部自由度。在低温下,自旋CFs在范围a_0 r ξ_c∝ T〜(-1/2)中以 ∝ 1 / r〜2衰减,其中a_0是晶格间距。我们模型中主要热力学量的分析结果与MC模拟非常相似,烧绿石晶格上经典Heisenberg模型(D = 3)的精确和分析结果。这表明棋盘格上的无限分量旋转矢量模型的基态是经典的旋转液体。

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