Phase diagram of the fully frustrated transverse-field Ising model on the honeycomb lattice
arXiv:1006.5287 · doi:10.1103/PhysRevB.83.054402
Abstract
Motivated by the current interest in the quantum dimer model on the triangular lattice, we investigate the phase diagram of the closely related fully-frustrated transverse field Ising model on the honeycomb lattice using classical and semi-classical approximations. We show that, in addition to the fully polarized phase at large field, the classical model possesses a multitude of phases that break the translational symmetry which in the dimer language, correspond to a plaquette phase and a columnar phase separated by an infinite cascade of mixed phases. The modification of the phase diagram by quantum fluctuations has been investigated in the context of linear spin-wave theory. The extrapolation of the semiclassical energies suggests that the plaquette phase extends down to zero field for spin 1/2, in agreement with the phase of the quantum dimer model on the triangular lattice with only kinetic energy.
15 Pages, 11 Figures, Accepted for PRB
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Cited by in corpus (11)
- Incomplete devil's staircase in the magnetization curve of SrCu2(BO3)2
- Quantum many-body scars in transverse field Ising ladders and beyond
- Topological phase transition and single/multi anyon dynamics of spin liquid
- Evidence of columnar order in the fully frustrated transverse field Ising model on the square lattice
- Spin-wave analysis of the transverse-field Ising model on the checkerboard lattice
- Selection of factorizable ground state in a frustrated spin tube: Order by disorder and hidden ferromagnetism
- Semiclassical evidence of columnar order in the fully frustrated transverse field Ising model on the square lattice
- Magnetic properties of a spin-orbit entangled Jeff = 1/2 honeycomb lattice
- Finite-temperature phase transitions in the quantum fully frustrated Ising models
- Sign-problem-free effective models of triangular lattice quantum antiferromagnets
- Continuous interpolation between the fully frustrated Ising and quantum dimer models