Plaquette order and deconfined quantum critical point in the spin-1 bilinear-biquadratic Heisenberg model on the honeycomb lattice

被引:58
|
作者
Zhao, H. H. [1 ]
Xu, Cenke [2 ]
Chen, Q. N. [3 ]
Wei, Z. C. [1 ]
Qin, M. P. [1 ]
Zhang, G. M. [4 ,5 ]
Xiang, T. [1 ,3 ]
机构
[1] Chinese Acad Sci, Inst Phys, Beijing 100190, Peoples R China
[2] Univ Calif Santa Barbara, Dept Phys, Santa Barbara, CA 93106 USA
[3] Chinese Acad Sci, Inst Theoret Phys, Beijing 100190, Peoples R China
[4] Tsinghua Univ, Dept Phys, Beijing 100084, Peoples R China
[5] Tsinghua Univ, State Key Lab Low Dimens Quantum Phys, Beijing 100084, Peoples R China
来源
PHYSICAL REVIEW B | 2012年 / 85卷 / 13期
关键词
TRIANGULAR-LATTICE; PHASE-TRANSITIONS; LIQUID STATE; DIMENSIONS; ANTIFERROMAGNETS;
D O I
10.1103/PhysRevB.85.134416
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We have precisely determined the ground state phase diagram of the quantum spin-1 bilinear-biquadratic Heisenberg model on the honeycomb lattice using the tensor renormalization group method. We find that the ferromagnetic, ferroquadrupolar, and a large part of the antiferromagnetic phases are stable against quantum fluctuations. However, around the phase where the ground state is antiferroquadrupolar ordered in the classical limit, quantum fluctuations suppress completely all magnetic orders, leading to a plaquette order phase which breaks the lattice symmetry but preserves the spin SU(2) symmetry. On the evidence of our numerical results, the quantum phase transition between the antiferromagnetic phase and the plaquette phase is found to be either a direct second order or a very weak first order transition.
引用
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页数:6
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