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Quantum Monte-Carlo study of magnetic ordering in ZnV_2O_4

机译:ZnV_2O_4磁性排序量子Quantum Monte-Carlo研究

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We study the magnetic ordering of Vanadium spinels by Quantum Monte Carlo simulations of a three-band Hubbard model. Vanadium spinels, AV_2O_4, exhibit a unique "up-up-down-down" spin ordering at low temperatures. While this magnetic ordering was originally measured in 1973, its origin has remained unclear for many years due to the lack of unbiased approaches for solving the relevant model. A three-band Hubbard model on the spinel lattice (corner sharing tetrahedra) is a minimal Hamiltonian for describing the t_(2g) electrons of the V~(2+) ions. One of the main difficulties is that this family of compounds belongs to the elusive intermediate-coupling regime (U ? t) for which there is no small parameter that can justify a perturbative expansion. We present a controlled Quantum Monte-Carlo approach to the three-band Hubbard model relevant for this materials that reproduces the up-up-down-down spin ordering. The method is free of the sign problem that is usually the main limiting factor for simulating fermionic systems in dimension higher than one.
机译:我们研究了三频段隆巴德模型的量子蒙特卡罗模拟钒尖晶石的磁性排序。钒尖晶石AV_2O_4,在低温下展示独特的“上下”旋转序命序。虽然这一磁性有序最初在1973年衡量,但由于缺乏用于解决相关模型的无偏见方法,其来源仍然不清楚多年。尖晶石格子(角落共享Tetrahedra)上的三频哈巴德型号是最小的Hamiltonian,用于描述V〜(2+)离子的T_(2G)电子。主要困难之一是,这家族化合物属于难以捉摸的中间耦合制度(U〜T),没有任何小参数可以证明扰动扩张。我们向3频段Monte-Carlo方法提出了一种与这种材料相关的三频哈巴德模型,该模型再现上下旋转排序。该方法没有符号问题,通常是模拟高于1的尺寸下的Fermionic系统的主要限制因素。

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