Classical model emerges in quantum entanglement: Quantum Monte Carlo study for an Ising-Heisenberg bilayer

被引:4
|
作者
Wu, Siying [1 ,2 ,3 ]
Ran, Xiaoxue [4 ,5 ]
Yin, Binbin [6 ]
Li, Qi-Fang [7 ]
Mao, Bin-Bin [8 ]
Wang, Yan-Cheng [3 ]
Yan, Zheng [4 ,5 ,9 ,10 ]
机构
[1] Fudan Univ, State Key Lab Surface Phys, Shanghai 200438, Peoples R China
[2] Fudan Univ, Dept Phys, Shanghai 200438, Peoples R China
[3] Beihang Hangzhou Innovat Inst Yuhang, Hangzhou 310023, Peoples R China
[4] Univ Hong Kong, Dept Phys, Pokfulam Rd, Hong Kong, Peoples R China
[5] Univ Hong Kong, HKU UCAS Joint Inst Theoret & Computat Phys, Pokfulam Rd, Hong Kong, Peoples R China
[6] City Univ Hong Kong, Dept Architecture & Civil Engn, Kowloon, Hong Kong, Peoples R China
[7] Univ Tokyo, Inst Solid State Phys, Chiba 2778581, Japan
[8] Univ Hlth & Rehabil Sci, Sch Fdn Educ, Qingdao 266071, Peoples R China
[9] Westlake Univ, Sch Sci, Dept Phys, 600 Dunyu Rd, Hangzhou 310030, Zhejiang, Peoples R China
[10] Westlake Inst Adv Study, Inst Nat Sci, 18 Shilongshan Rd, Hangzhou 310024, Zhejiang, Peoples R China
基金
日本科学技术振兴机构;
关键词
ENTROPY;
D O I
10.1103/PhysRevB.107.155121
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
By developing a cluster sampling of the stochastic series expansion quantum Monte Carlo method, we investigate a spin -21 model on a bilayer square lattice with intralayer ferromagnetic (FM) Ising coupling and interlayer antiferromagnetic Heisenberg interaction. The continuous quantum phase transition which occurs at gc = 3.045(2) between the FM Ising phase and the dimerized phase is studied via large-scale simulations. From analysis of the critical exponents we show that this phase transition belongs to the (2+1)-dimensional Ising universality class. In addition, the quantum entanglement is strong between the two layers, especially in the dimerized phase. The effective Hamiltonian of a single layer seems like a transverse-field Ising model. However, we found that the quantum entanglement Hamiltonian is a pure classical Ising model without any quantum fluctuations. Furthermore, we give a more general explanation about how a classical entanglement Hamiltonian emerges.
引用
收藏
页数:8
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