paper

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

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