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电子 - 空穴掺杂哈伯德双层中的双激子凝聚:无符号问题的量子蒙特卡罗研究

Biexciton Condensation in Electron-Hole-Doped Hubbard Bilayers: A Sign-Problem-Free Quantum Monte Carlo Study.

作者信息

Huang Xu-Xin, Claassen Martin, Huang Edwin W, Moritz Brian, Devereaux Thomas P

机构信息

Department of Applied Physics, Stanford University, Stanford, California 94305, USA.

Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory and Stanford University, 2575 Sand Hill Road, Menlo Park, California 94025, USA.

出版信息

Phys Rev Lett. 2020 Feb 21;124(7):077601. doi: 10.1103/PhysRevLett.124.077601.

Abstract

The bilayer Hubbard model with electron-hole doping is an ideal platform to study excitonic orders due to suppressed recombination via spatial separation of electrons and holes. However, suffering from the sign problem, previous quantum Monte Carlo studies could not arrive at an unequivocal conclusion regarding the presence of phases with clear signatures of excitonic condensation in bilayer Hubbard models. Here, we develop a determinant quantum Monte Carlo algorithm for the bilayer Hubbard model that is sign-problem-free for equal and opposite doping in the two layers and study excitonic order and charge and spin density modulations as a function of chemical potential difference between the two layers, on-site Coulomb repulsion, and interlayer interaction. In the intermediate coupling regime and in proximity to the SU(4)-symmetric point, we find a biexcitonic condensate phase at finite electron-hole doping, as well as a competing (π,π) charge density wave state. We extract the Berezinskii-Kosterlitz-Thouless transition temperature from superfluid density and a finite-size scaling analysis of the correlation functions and explain our results in terms of an effective biexcitonic hard-core boson model.

摘要

具有电子 - 空穴掺杂的双层哈伯德模型是研究激子序的理想平台,因为电子和空穴的空间分离抑制了复合。然而,由于存在符号问题,先前的量子蒙特卡罗研究未能就双层哈伯德模型中具有明显激子凝聚特征的相的存在得出明确结论。在此,我们为双层哈伯德模型开发了一种行列式量子蒙特卡罗算法,该算法对于两层中相等且相反的掺杂是无符号问题的,并研究了激子序以及电荷和自旋密度调制作为两层之间化学势差、在位库仑排斥和层间相互作用的函数。在中间耦合区域且接近SU(4)对称点时,我们在有限电子 - 空穴掺杂下发现了一个双激子凝聚相,以及一个与之竞争的(π,π)电荷密度波态。我们从超流密度以及关联函数的有限尺寸标度分析中提取了贝雷津斯基 - 科斯特利茨 - Thouless转变温度,并根据有效的双激子硬核玻色子模型解释了我们的结果。

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