Singular ferromagnetic susceptibility of the transverse-field Ising antiferromagnet on the triangular lattice
arXiv:1603.06473 · doi:10.1103/PhysRevB.97.085114
Abstract
A transverse magnetic field is known to induce antiferromagnetic three-sublattice order of the Ising spins in the triangular lattice Ising antiferromagnet at low enough temperature. This low-temperature order is known to melt on heating in a two-step manner, with a power-law ordered intermediate temperature phase characterized by power-law correlations at the three-sublattice wavevector : with the temperature-dependent power-law exponent . Here, we use a newly developed quantum cluster algorithm to study the {\em ferromagnetic} easy-axis susceptibility of an sample in this power-law ordered phase. Our numerical results are consistent with a recent prediction of a singular dependence when is in the range . This finite-size result implies, via standard scaling arguments, that the ferromagnetic susceptibility to a uniform field along the easy axis is singular at intermediate temperatures in the small limit, for , although there is no ferromagnetic long-range order in the low temperature state.
8 two-column pages; 10 figures
References in corpus (4)
- Stochastic series expansion method for quantum Ising models with arbitrary interactions
- Interplay of quantum and thermal fluctuations in a frustrated magnet
- Melting of three-sublattice order in easy-axis antiferromagnets on triangular and Kagome lattices
- Quantum cluster algorithm for frustrated Ising models in a transverse field
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- Intrinsic transverse field in frustrated quantum Ising magnets: its physical origin and quantum effects
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- Two-step melting of three-sublattice order in easy-axis triangular lattice antiferromagnets
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