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在正方晶格交错磁通 Hubbard 模型中 Mott 转变附近的量子无序相。

Quantum disordered phase near the Mott transition in the staggered-flux Hubbard model on a square lattice.

机构信息

Department of Physics, University of California, Davis, Davis, California 95616, USA.

出版信息

Phys Rev Lett. 2012 Jul 13;109(2):026404. doi: 10.1103/PhysRevLett.109.026404.

Abstract

We investigate ground state properties of the half-filled staggered-flux Hubbard model on a square lattice. Energy gaps to charge and spin excitations and magnetic as well as dimer orders are calculated as a function of interaction strength U/t by means of a constrained-path quantum Monte Carlo method. It is found that the system is a semimetal at U/t≲5.6 and a Mott insulator, with long-range antiferromagnetic order, at U/t≳6.6. In the range 5.6≲U/t≲6.6, the ground state is a correlated insulator where both magnetic and dimer orders are absent. Furthermore, spin excitation in the intermediate phase appears to be gapless, and the measured spin-spin correlation function exhibits power-law decaying behavior. The data suggest that the nonmagnetic ground state is a possible candidate for the putative algebraic spin liquid.

摘要

我们研究了正方晶格上半填满交错磁通 Hubbard 模型的基态性质。通过受限路径量子蒙特卡罗方法,计算了电荷和自旋激发、磁有序和二聚体有序的能隙作为相互作用强度 U/t 的函数。结果发现,当 U/t≲5.6 时,系统为半金属,当 U/t≳6.6 时,系统为莫特绝缘体,具有长程反铁磁序。在 5.6≲U/t≲6.6 的范围内,基态为关联绝缘态,不存在磁有序和二聚体有序。此外,中间相中的自旋激发似乎是无能隙的,测量得到的自旋-自旋相关函数呈现出幂律衰减行为。这些数据表明,非磁性基态可能是假设的代数自旋液体的候选物。

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