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The frustrated Heisenberg antiferromagnet on the honeycomb lattice: A candidate for deconfined quantum criticality

Abstract

We study the ground-state (gs) phase diagram of the frustrated spin-1/2 J1J_{1}-J2J_{2}-J3J_{3} antiferromagnet with J2=J3=κJ1J_{2} = J_{3} =\kappa J_1 on the honeycomb lattice, using coupled-cluster theory and exact diagonalization methods. We present results for the gs energy, magnetic order parameter, spin-spin correlation function, and plaquette valence-bond crystal (PVBC) susceptibility. We find a N\'eel antiferromagnetic (AFM) phase for κ<κc10.47\kappa < \kappa_{c_{1}} \approx 0.47, a collinear striped AFM phase for κ>κc20.60\kappa > \kappa_{c_{2}} \approx 0.60, and a paramagnetic PVBC phase for κc1κκc2\kappa_{c_{1}} \lesssim \kappa \lesssim \kappa_{c_{2}}. The transition at κc2\kappa_{c_{2}} appears to be of first-order type, while that at κc1\kappa_{c_{1}} is continuous. Since the N\'eel and PVBC phases break different symmetries our results favor the deconfinement scenario for the transition at κc1\kappa_{c_{1}}

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