Spin wavepacket propagation in quasi-2D antiferromagnets

TL;DR

This paper explains the unexpectedly high and anisotropic spin wavepacket velocities in quasi-2D antiferromagnets through dipole-dipole interactions, showing they can be tuned by external fields and sample thickness, and explores implications for Bose-Einstein condensation.

Contribution

It reveals the role of long-range dipolar interactions in spin wave dynamics and demonstrates tunability, expanding understanding of antiferromagnetic spin wave propagation.

Findings

Dipolar interactions explain anomalous group velocities.

External magnetic fields and thickness control velocity.

Potential for non-equilibrium Bose-Einstein condensation.

Abstract

Antiferromagnets are attractive platforms for the propagation of information via spin waves, offering advantages over ferromagnets in speed of response and immunity to external fields. A recent study of the quasi-2D antiferromagnet CrSBr reported that spin wavepackets propagate with group velocities that are orders of magnitude higher than expected from the magnon dispersion obtained by inelastic neutron scattering [1,2]. Here we show that the anomalous magnitude and anisotropy of the group velocity, v_g, are naturally explained by considering the long-range magnetic dipole-dipole interaction. We also demonstrate that v_g can be tuned over orders of magnitude by applying an external magnetic field or varying the sample thickness. Beyond spin wavepacket propagation, the dipolar interaction creates the possibility of non-equilibrium Bose-Einstein condensation in antiferromagnets, previously thought to be a property unique to ferromagnets.