Abstract
We report measurements of the magnetic excitation spectrum of the layered antiferromagnet ${\text{La}}_{2}{\text{CoO}}_{4}$ by time-of-flight neutron inelastic scattering. In the energy range probed in our experiments (0--250 meV) the magnetic spectrum consists of spin-wave modes with strong in-plane dispersion extending up to 60 meV, and a nearly dispersionless peak at 190 meV. The spin-wave modes exhibit a small $(\ensuremath{\sim}1\text{ }\text{meV})$ dispersion along the magnetic zone boundary. We show that the magnetic spectrum can be described very well by a model of a Heisenberg antiferromagnet that includes the full spin and orbital degrees of freedom of ${\text{Co}}^{2+}$ in an axially distorted crystal field. The collective magnetic dynamics are found to be controlled by dominant nearest-neighbor exchange interactions, strong XY-like single-ion anisotropy and a substantial unquenched orbital angular momentum.
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