Plaquette Ordered Phase and Quantum Phase Diagram in the Spin-1/2 J1-J2 Square Heisenberg Model

被引:220
|
作者
Gong, Shou-Shu [1 ]
Zhu, Wei [1 ]
Sheng, D. N. [1 ]
Motrunich, Olexei I. [2 ]
Fisher, Matthew P. A. [3 ]
机构
[1] Calif State Univ Northridge, Dept Phys & Astron, Northridge, CA 91330 USA
[2] CALTECH, Dept Phys, Pasadena, CA 91125 USA
[3] Univ Calif Santa Barbara, Dept Phys, Santa Barbara, CA 93106 USA
基金
美国国家科学基金会;
关键词
MEAN-FIELD THEORY; ENTANGLEMENT ENTROPY; TOPOLOGICAL ORDER; LIQUID; ANTIFERROMAGNET; LATTICE; SYSTEMS; STATES; SPINS;
D O I
10.1103/PhysRevLett.113.027201
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We study the spin-1/2 Heisenberg model on the square lattice with first-and second-neighbor antiferromagnetic interactions J(1) and J(2), which possesses a nonmagnetic region that has been debated for many years and might realize the interesting Z(2) spin liquid. We use the density matrix renormalization group approach with explicit implementation of SU(2) spin rotation symmetry and study the model accurately on open cylinders with different boundary conditions. With increasing J(2), we find a Neel phase and a plaquette valence-bond (PVB) phase with a finite spin gap. From the finite-size scaling of the magnetic order parameter, we estimate that the Neel order vanishes at J(2) = J(1) similar or equal to 0.44. For 0.5 < J(2)/J(1) < 0.61, we find dimer correlations and PVB textures whose decay lengths grow strongly with increasing system width, consistent with a long-range PVB order in the two-dimensional limit. The dimer-dimer correlations reveal the s-wave character of the PVB order. For 0.44 < J(2)/J(1) < 0.5, spin order, dimer order, and spin gap are small on finite-size systems, which is consistent with a near-critical behavior. The critical exponents obtained from the finite-size spin and dimer correlations could be compatible with the deconfined criticality in this small region. We compare and contrast our results with earlier numerical studies.
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页数:5
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