Entanglement negativity via the replica trick: A quantum Monte Carlo approach

被引:49
|
作者
Chung, Chia-Min [1 ,2 ]
Alba, Vincenzo [3 ,4 ]
Bonnes, Lars [5 ]
Chen, Pochung [1 ,2 ,6 ]
Laeuchli, Andreas M. [5 ]
机构
[1] Natl Tsing Hua Univ, Dept Phys, Hsinchu 30013, Taiwan
[2] Natl Tsing Hua Univ, Frontier Res Ctr Fundamental & Appl Sci Matters, Hsinchu 30013, Taiwan
[3] Univ Munich, Dept Phys, D-80333 Munich, Germany
[4] Univ Munich, Arnold Sommerfeld Ctr Theoret Phys, D-80333 Munich, Germany
[5] Univ Innsbruck, Inst Theoret Phys, A-6020 Innsbruck, Austria
[6] Natl Ctr Theoret Sci, Div Phys, Hsinchu 30013, Taiwan
基金
奥地利科学基金会;
关键词
ENTROPY;
D O I
10.1103/PhysRevB.90.064401
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Motivated by recent developments in conformal field theory (CFT), we devise a quantum Monte Carlo (QMC) method to calculate the moments of the partially transposed reduced density matrix at finite temperature. These are used to construct scale invariant combinations that are related to the negativity, a true measure of entanglement for two intervals embedded in a chain. These quantities can serve as witnesses of criticality. In particular, we study several scale invariant combinations of the moments for the one-dimensional (1D) hard-core boson model. For two adjacent intervals unusual finite-size corrections are present, showing parity effects that oscillate with a filling dependent period. These are more pronounced in the presence of boundaries. For large chains we find perfect agreement with CFT. Oppositely, for disjoint intervals corrections are more severe and CFT is recovered only asymptotically. Furthermore, we provide evidence that their exponent is the same as that governing the corrections of the mutual information. Additionally we study the 1D Bose-Hubbard model in the superfluid phase. Remarkably, the finite-size effects are smaller and QMC data are already in impressive agreement with CFT at moderately large sizes.
引用
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页数:6
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