Published March 26, 2024 | Version v1
Journal article

Chiral spin liquid and quantum phase diagram of spin-12 J1J2Jχ model on the square lattice

  • 1. School of Physics, Beihang University, Beijing 100191, China
  • 2. Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 3. Center for Integrated Nanotechnologies, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 4. Guangdong Provincial Key Laboratory of Magnetoelectric Physics and Devices, School of Physics, Sun Yat-sen University, Guangzhou 510275, China
  • 5. Department of Physics and Astronomy, California State University Northridge, Northridge, California 91330, USA
  • 6. School of Physical Sciences, Great Bay University, Dongguan 523000, China
  • 7. Great Bay Institute for Advanced Study, Dongguan 523000, China

Description

We study the spin-1/2 Heisenberg model on the square lattice with the first- and second-nearest-neighbor antiferromagnetic couplings J1 and J2, as well as the three-spin scalar chiral coupling Jχ. Using density matrix renormalization group calculations, we obtain a quantum phase diagram of this system for 0J2/J11.0 and 0Jχ/J11.5. We identify the Néel and stripe magnetic order phase at small-Jχ coupling. With growing Jχ, we identify the emergent chiral spin liquid (CSL) phase characterized by the quantized spin Chern number C=1/2 and entanglement spectrum with the quasidegenerate group of levels agreeing with chiral SU(2)1 conformal field theory, which is an analog of the ν=1/2 Laughlin state in the spin system. In the vicinity of the Néel and CSL phase boundary, our numerical results do not find evidence to support the coexistence of Néel order and topological order that was conjectured by mean-field calculations. In the larger-J2 and -Jχ coupling regime, the entanglement spectrum of the ground state also exhibits the chiral quasidegeneracy consistent with a CSL, but the adiabatic flux insertion simulations fail to obtain the quantized Chern number. By analyzing the finite-size scaling of the magnetic order parameter, we find the vanished magnetic order suggesting a magnetic disorder phase, whose nature needs further studies. Different from the spin-1J1J2Jχ model, we do not find the coexistent stripe magnetic order and topological order. We also investigate the Jχ dominant regime and find a strong tendency of the system to develop a dimer order rather than the chiral spin magnetic order observed in the spin-1 model. Our results unveil interesting quantum phases in this spin-1/2 model and also demonstrate the drastic differences between the spin-1/2 and spin-1 cases.

Additional details

Identifiers

DOI
10.1103/PhysRevB.109.125146;
arXiv
arXiv:2401.07461;
Crossref Funder ID
10.13039/501100001809; 10.13039/100000015;

Publishing Information

Journal Title
Physical Review B
Journal Volume
109
Journal Issue
12
Journal Page Range
15 pgs.
ISSN
1550-235X

Optional Information

Copyright
©2024 American Physical Society
Contract/Grant/Project number
11874078; 11834014; 89233218CNA000001
Notes
Contact Email: wuhanq3@mail.sysu.edu.cn; Contact Email: donna.sheng1@csun.edu; Contact Email: shoushu.gong@gbu.edu.cn; Record automatically processed
Funding organization
National Natural Science Foundation of China; U.S. Department of Energy