Schwinger Boson mean field theory of kagome Heisenberg antiferromagnet with Dzyaloshinskii-Moriya interaction
arXiv:2001.10711 · doi:10.1103/PhysRevB.95.134404
Abstract
We have studied the effect of the Dzyaloshinskii-Moriya interaction on kagome Heisenberg anti-ferromagnet using Schwinger boson mean field theory (SBMFT). Within SBMFT framework, Messio et al had argued that the ground state of kagome antiferromagnet is possibly a chiral topological spin liquid (Phys. Rev. Lett. 108, 207204 (2012)). Thus, we have computed zero-temperature ground state phase diagram considering the time-reversal breaking states as well as fully symmetric Ansätze. We discuss the relevance of these results in experiments and other studies. Finally, we have computed the static and dynamic spin structure factors in relevant phases.
References in corpus (12)
- Spin Dynamics of the Spin-1/2 Kagome Lattice Antiferromagnet ZnCu_3(OH)_6Cl_2
- Projected wavefunction study of Spin-1/2 Heisenberg model on the Kagome lattice
- Properties of an algebraic spin liquid on the kagome lattice
- Spin Liquid States on the Triangular and Kagome Lattices: A Projective Symmetry Group Analysis of Schwinger Boson States
- Quantum phase transition induced by Dzyaloshinskii-Moriya in the kagome antiferromagnet
- Dzyaloshinsky-Moriya Anisotropy in the Spin-1/2 Kagomé Compound ZnCu(OH)Cl
- Magnetic Susceptibility of the Kagome Antiferromagnet ZnCu3(OH)6Cl2
- Time-reversal-symmetry-breaking chiral spin liquids: a projective symmetry group approach of bosonic mean-field theories
- Symplectic N and time reversal in frustrated magnetism
- Quantum criticality of the kagome antiferromagnet with Dzyaloshinskii-Moriya interactions
- Dzyaloshinskii-Moriya anisotropy and non-magnetic impurities in the kagome system ZnCu_3(OH)_6Cl_2
- Dzyaloshinskii-Moriya interactions in valence bond systems