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量子蒙特卡罗模拟受挫的康顿晶格模型。

Quantum Monte Carlo Simulation of Frustrated Kondo Lattice Models.

机构信息

Institut für Theoretische Physik und Astrophysik, Universität Würzburg, 97074 Würzburg, Germany.

Department of Physics, University of California at San Diego, La Jolla, California 92093, USA.

出版信息

Phys Rev Lett. 2018 Mar 9;120(10):107201. doi: 10.1103/PhysRevLett.120.107201.

Abstract

The absence of the negative sign problem in quantum Monte Carlo simulations of spin and fermion systems has different origins. World-line based algorithms for spins require positivity of matrix elements whereas auxiliary field approaches for fermions depend on symmetries such as particle-hole symmetry. For negative-sign-free spin and fermionic systems, we show that one can formulate a negative-sign-free auxiliary field quantum Monte Carlo algorithm that allows Kondo coupling of fermions with the spins. Using this general approach, we study a half-filled Kondo lattice model on the honeycomb lattice with geometric frustration. In addition to the conventional Kondo insulator and antiferromagnetically ordered phases, we find a partial Kondo screened state where spins are selectively screened so as to alleviate frustration, and the lattice rotation symmetry is broken nematically.

摘要

自旋和费米子系统的量子蒙特卡罗模拟中不存在负号问题,其起源也各不相同。基于世界线的自旋算法要求矩阵元为正,而对于费米子的辅助场方法则依赖于粒子-空穴对称性等对称性。对于无负号的自旋和费米子系统,我们表明可以制定一种无负号的辅助场量子蒙特卡罗算法,允许费米子与自旋的康顿耦合。使用这种通用方法,我们研究了具有几何各向异性的蜂窝晶格上的半满康顿晶格模型。除了传统的康顿绝缘相和反铁磁有序相之外,我们还发现了一种部分康顿屏蔽态,其中自旋被选择性地屏蔽以减轻各向异性,晶格旋转对称性被向列性破坏。

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