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Quantum paramagnetic ground states on the honeycomb lattice and field-induced transition to N\'eel order

Abstract

Motivated by recent experiments on Bi3_3Mn4_4O12_{12}(NO3_3), and a broader interest arising from numerical work on the honeycomb lattice Hubbard model, we have studied the effect of a magnetic field on honeycomb lattice spin models with quantum paramagnetic ground states. For a model with frustrating second-neighbor exchange, J2J_2, we use a Lindemann-like criterion within spin wave theory to show that N\'eel order melts beyond a critical J2J_2. The critical J2J_2 increases with a magnetic field, implying the existence of a field-induced paramagnet-N\'eel transition over a range of J2J_2. We also study bilayer model using a spin-SS generalization of bond operator mean field theory. We show that there is a N\'eel-dimer transition for various spin values with increasing bilayer coupling, and that the resulting interlayer dimer state undergoes a field induced transition into a state with transverse N\'eel order. Finally, we study a spin-3/2 model which interpolates between the Heisenberg model and the Affleck-Kennedy-Lieb-Tasaki (AKLT) parent Hamiltonian. Using exact diagonalization, we compute the fidelity susceptibility to locate the Neel-AKLT quantum critical point, obtain the spin gap of the AKLT parent Hamiltonian, and argue that AKLT state also undergoes field-induced Neel ordering.Comment: 8 pages, revised longer version of arXiv:1012.0316. Corrected factor of 2 error in Eq.[16], replotted Fig.[4] and revised the critical Jc/J1J_c/J_1 needed to stabilize interlayer dimer state. We thank S. V. Isakov for discussions which uncovered this erro

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