Transverse Magnetic Susceptibility of a Frustrated Spin- ---- Heisenberg Antiferromagnet on a Bilayer Honeycomb Lattice
arXiv:1709.08205 · doi:10.1063/1.5016136
Abstract
We use the coupled cluster method (CCM) to study a frustrated spin- ---- Heisenberg antiferromagnet on a bilayer honeycomb lattice with stacking. Both nearest-neighbor (NN) and frustrating next-nearest-neighbor antiferromagnetic (AFM) exchange interactions are present in each layer, with respective exchange coupling constants and . The two layers are coupled with NN AFM exchanges with coupling strength . We calculate to high orders of approximation within the CCM the zero-field transverse magnetic susceptibility in the Néel phase. We thus obtain an accurate estimate of the full boundary of the Néel phase in the plane for the zero-temperature quantum phase diagram. We demonstrate explicitly that the phase boundary derived from is fully consistent with that obtained from the vanishing of the Néel magnetic order parameter. We thus conclude that at all points along the Néel phase boundary quasiclassical magnetic order gives way to a nonclassical paramagnetic phase with a nonzero energy gap. The Néel phase boundary exhibits a marked reentrant behavior, which we discuss in detail.
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