Abstract

We report on the theoretical prediction of asymmetric edge spin waves, propagating in opposite directions at the boundaries of antiferromagnetic honeycomb nanoribbons with zigzag and bearded edges. The simultaneous propagation of edge spin waves along the same direction on both edges of the nanoribbons is forbidden. These asymmetric exchange spin waves at the edge boundaries are analogous to the nonreciprocal surface spin waves reported in magnetic thin films. Their existence is related to the nontrivial symmetry underlying these nanoribbons types. The discretized bulk and the edge exchange spin waves are calculated for the long wavelength part of the nanoribbon Brillouin zone (BZ), using the classical field spin wave theory and notably appropriate boundary conditions. In the absence of an external magnetic field in our study, the asymmetric edge spin waves propagate with equal frequencies and along opposite directions. The edge spin waves are characterized by linear dispersion relations for magnetically isotropic nanoribbons. For magnetically anisotropic nanoribbons, our calculations show that the energy gap between the edge and bulk spin waves is enhanced for both types of zigzag and bearded nanoribbons. The large energy gap separates the edge modes from overlapping the bulk ones. Also, we explain why our results for anisotropic zigzag nanoribbons go beyond previous studies based on a quantum approach in the linear spin wave approximation.

Highlights

  • Despite its broad success in the study of surface spin waves, the classical field theory has not been systematically developed for edge spin waves in 2D materials until our recent study of long wavelength exchange spin waves on 2D antiferromagnetic nanoribbons with armchair edge boundaries[54]

  • We further develop the classical spin waves approach and apply it to study the bulk and edge exchange spin waves in 2D antiferromagnetic nanoribbons with zigzag and bearded edge boundaries, in the long wavelength part of the Brillouin zone (BZ)

  • The allowed values of ky are different for the two nanoribbon types, since the d values for the nanoribbon half width are structurally different for zigzag and bearded edge nanoribbons

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Summary

Methods

We consider a semi-classical Heisenberg Hamiltonian with exchange interaction between the spins. + Sy yrepresents the spin component in the plane of the Bloch equations of motion for the magnetization the honeycomb →A →B M and M of lattice. The honeycomb sublattices[54], the bulk wave equation describing the spin waves dynamics can be derived as. Compared to previous studies[28,45,46,52], we here adopt a more general form for the solutions, suitable for bounded systems where both e±qy terms are physical. The real and imaginary values of q correspond respectively to evanescent (edge), and propagating (bulk), spin waves in the y-direction along which the nanoribbon is finite. Substituting equations (2) in the bulk wave Eq (1) yields the dispersion relation. This (4) hold for any y along yields the relations the width of the nanoribbon

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