The two-dimensional (2D) frustrated honeycomb Heisenberg antiferromagnet can support several kinds of ground states according to the ratio α = J2/J1. Understanding these states is a central challenge in quantum magnetism.
Figure: Crystal structure and magnetic connectivity in Cu5SbO6.
By comparing experimental dispersion relations with theoretical models, we can justify whether observations align with predictions of Neel order, plaquette resonating valence bonds, or dimer ground states.