Paramagnetic Acoustic Faraday Rotation in Tb3Ga5O12

TL;DR

This paper presents a new model explaining the acoustic Faraday rotation in Tb3Ga5O12, accounting for its linear frequency dependence and magnetic field resonance, resolving a long-standing theoretical discrepancy.

Contribution

The authors propose a magnetoelastic interaction model involving optical phonons to explain the linear frequency dependence of the acoustic Faraday rotation.

Findings

Rotation angle varies linearly with frequency, matching experimental observations.

The model explains the resonance in the 17-20 T magnetic field range.

It provides a general mechanism applicable to non-Bravais lattices.

Abstract

The acoustic Faraday rotation in the 4f paramagnet Tb3Ga5O12 has recently been observed by Sytcheva et al (arXiv:1006.0141). As in earlier examples the rotation angle per unit length of transverse acoustic modes was found to depend linearly on sound frequency. Existing theories for this effect consistently require that it should vary with the square of the frequency. In the present work a solution for this long-standing problem is provided. We propose a model based on magnetoelastic interactions with 4f quadrupole moments that includes both acoustic and optical phonons. The symmetry allows a direct and induced coupling between the latter. This leads to an indirect acoustic Faraday rotation via the field induced splitting of doubly degenerate optical phonon modes. It varies linearly with frequency in accordance with experiment and dominates the rotation angle. It also explains the observed resonance of the rotation angle in the field range between 17-20 T. The mechanism is of general validity for non-Bravais lattices and applies to previous examples of the acoustic Faraday effect.