Abstract

Magneto-structural phase transition in FeRh epitaxial layers was studied optically. It is shown that the transition between the low-temperature antiferromagnetic phase and the high-temperature ferromagnetic phase is accompanied by a rather large change of the optical response in the visible and near-infrared spectral ranges. This change is consistent with ab initio calculations of reflectivity and transmittance. Phase transition temperatures in a series of FeRh films with thicknesses ranging from 6 to 100 nm is measured thereby demonstrating the utility of the method to quickly characterise samples. Spatially resolved imaging of their magnetic properties with a micrometer resolution shows that the phase transition occurs at different temperatures in different parts of the sample.

Highlights

  • The near-equiatomic alloy of iron and rhodium undergoes a first-order magneto-structural transition from an antiferromagnetic (AF) to ferromagnetic (FM) phase around 380 K

  • We show that the AF to FM phase transition can be studied by the most straightforward optical experiment where the sample transmission and/or reflectivity is measured while the sample temperature is varied

  • Contrary to previous claims [17], we observe a clear change of optical properties of FeRh thin films upon crossing the AF to FM transition and find it to be most significantly pronounced in the near infrared spectral range

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Summary

August 2016

It is shown that the transition between the low-temperature antiferromagnetic phase and the high-temperature ferromagnetic phase is accompanied by a rather large change of the optical response in the visible and near-infrared spectral ranges. This change is consistent with ab initio calculations of reflectivity and transmittance. Resolved imaging of their magnetic properties with a micrometer resolution shows that the phase transition occurs at different temperatures in different parts of the sample

Introduction
Samples and experimental setup
Reflectivity and transmittance: measurement and ab initio modelling
Spatially resolved measurements
Findings
Conclusions

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