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