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三维 Hubbard 模型中的磁有序和向二维的交叉。

Magnetic order in the Hubbard model in three dimensions and the crossover to two dimensions.

机构信息

Department of Physics, College of William and Mary, Williamsburg, VA 23187, USA.

出版信息

J Phys Condens Matter. 2013 Oct 16;25(41):415602. doi: 10.1088/0953-8984/25/41/415602. Epub 2013 Sep 18.

Abstract

Systems of fermions described by the three-dimensional (3D) repulsive Hubbard model on a cubic lattice have recently attracted considerable attention due to their possible experimental realization via cold atoms in an optical lattice. Analytical and numerical results are limited away from half-filling. We study the ground state of the doped system from weak to intermediate interaction strengths within the generalized Hartree-Fock approximation. The exact solution to the self-consistent-field equations in the thermodynamic limit is obtained and the ground state is shown to exhibit antiferromagnetic order and incommensurate spin-density waves (SDW). At low interaction strengths, the SDW has unidirectional character with a leading wavevector along the [100]-direction, and the system is metallic. As the interaction increases, the system undergoes a simultaneous structural and metal-to-insulator transition to a unidirectional SDW state along the [111]-direction, with a different wavelength. We systematically determine the real and momentum space properties of these states. The crossover from 3D to two dimensions (2D) is then studied by varying the inter-plane hopping amplitude, which can be experimentally realized by tuning the distance between a stack of square-lattice layers. Detailed comparisons are made between the exact numerical results and predictions from the pairing model, a variational ansatz based on the pairing of spins in the vicinity of the Fermi surface. Most of the numerical results can be understood quantitatively from the ansatz, which provides a simple picture for the nature of the SDW states.

摘要

由于通过冷原子在光晶格中的实验实现的可能性,最近,在立方格子上的三维(3D)排斥 Hubbard 模型描述的费米子系统引起了相当大的关注。远离半满时,分析和数值结果受到限制。我们在广义哈特ree-Fock 近似内研究了掺杂系统在弱到中等相互作用强度下的基态。在热力学极限下,获得了自洽场方程的精确解,并且显示基态表现出反铁磁序和非共调自旋密度波(SDW)。在低相互作用强度下,SDW 具有单向特征,主导波矢沿[100]-方向,并且系统是金属的。随着相互作用的增加,系统经历了结构和金属-绝缘体的同时转变,沿[111]-方向具有单向 SDW 状态,具有不同的波长。我们系统地确定了这些状态的实空间和动量空间特性。然后通过改变层间跃迁振幅来研究从 3D 到二维(2D)的转变,层间跃迁振幅可以通过调节正方形层堆栈之间的距离来实验实现。我们对精确数值结果和配对模型的预测进行了详细比较,配对模型是基于费米面附近的自旋配对的变分假设。大多数数值结果可以从假设中进行定量理解,这为 SDW 状态的性质提供了一个简单的图景。

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