Abstract
We study the ground-state (gs) phase diagram of the frustrated spin-1/2 J1–J2–J3 antiferromagnet with J2 = J3 = κ J1 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 < κc1 ≈ 0.47, a collinear striped AFM phase for κ > κc2 ≈ 0.60, and a paramagnetic PVBC phase for κc1 ≤ κ ≤ κc2 . The transition at κc2 appears to be of first-order type, while that at κc1 is continuous. Since the N´eel and PVBC phases break different symmetries our results favor the deconfinement scenario for the transition at κc1 .
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 < κc1 ≈ 0.47, a collinear striped AFM phase for κ > κc2 ≈ 0.60, and a paramagnetic PVBC phase for κc1 ≤ κ ≤ κc2 . The transition at κc2 appears to be of first-order type, while that at κc1 is continuous. Since the N´eel and PVBC phases break different symmetries our results favor the deconfinement scenario for the transition at κc1 .
Original language | English |
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Article number | 012403 (4pp) |
Journal | Physical Review B (Condensed Matter and Materials Physics) |
Volume | 84 |
DOIs | |
Publication status | Published - 2011 |