Dynamical properties of Néel and valence-bond phases in the model on the honeycomb lattice
arXiv:1912.09310 · doi:10.1088/1361-648X/ab7f6e
Abstract
By using a variational Monte Carlo technique based upon Gutzwiller-projected fermionic states, we investigate the dynamical structure factor of the antiferromagnetic Heisenberg model on the honeycomb lattice, in presence of first-neighbor () and second-neighbor () couplings, for . The ground state of the system shows long-range antiferromagnetic order for , plaquette valence-bond order for , and columnar dimer order for . Within the antiferromagnetic state, a well-defined magnon mode is observed, whose dispersion is in relatively good agreement with linear spin-wave approximation for . When a nonzero second-neighbor super-exchange is included, a roton-like mode develops around the point (i.e., the corner of the Brillouin zone). This mode softens when is increased and becomes gapless at the transition point, . Here, a broad continuum of states is clearly visible in the dynamical spectrum, suggesting that nearly-deconfined spinon excitations could exist, at least at relatively high energies. For larger values of , valence-bond order is detected and the spectrum of the system becomes clearly gapped, with a triplon mode at low energies. This is particularly evident for the spectrum of the dimer valence-bond phase, in which the triplon mode is rather well separated from the continuum of excitations that appears at higher energies.
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