Abstract

Magnetic anisotropy is a fundamental key parameter of magnetic materials that determines their applications. For ferromagnetic materials, the magnetic anisotropy can be easily detected by using conventional magnetic characterization techniques. However, due to the magnetic compensated structure in antiferromagnetic materials, synchrotron measurements, such as X-ray magnetic linear dichroism, are often needed to probe their magnetic properties. In this work, we observed an imprinted fourfold magnetic anisotropy in the amorphous ferromagnetic layer of FeRh/CoFeB heterostructures. The MOKE and ferromagnetic resonance measurements show that the easy magnetization axes of the CoFeB layer are along the FeRh〈110〉 and FeRh〈100〉 directions for the epitaxially grown FeRh layer in the antiferromagnetic and ferromagnetic states, respectively. The combined Monte Carlo simulation and first-principles calculation indicate that the fourfold magnetic anisotropy of the amorphous CoFeB layer is imprinted due to the interfacial exchange coupling between the CoFeB and FeRh moments from the magnetocrystalline anisotropy of the epitaxial FeRh layer. This observation of imprinting the magnetocrystalline anisotropy of antiferromagnetic materials on easily detected ferromagnetic materials may be applied to probe the magnetic structures of antiferromagnetic materials without using synchrotron methods.

Highlights

  • Magnetic anisotropy is a fundamental key parameter of magnetic materials, which determines the application of various magnetic materials1

  • It is of great interest that the amorphous CoFeB layer displays an in-plane fourfold magnetic anisotropy, which is usually observed in single crystal films

  • The magneto-optical Kerr effect (MOKE) and FM resonance (FMR) measurements indicate that the amorphous CoFeB layer displays an in-plane fourfold magnetic anisotropy, which is usually observed in single crystal films

Read more

Summary

Introduction

Magnetic anisotropy is a fundamental key parameter of magnetic materials, which determines the application of various magnetic materials. A soft magnetic material needs a magnetic anisotropy as weak as possible to reduce the hysteresis loss. Extrinsic magnetic anisotropy is usually induced by the shape of the magnetic materials, the applied stress, the processing techniques, and the interfacial exchange coupling. 60 years ago by Meiklejohn and Bean in a composite system containing an FM material coupled with the adjacent AF material. 60 years ago by Meiklejohn and Bean in a composite system containing an FM material coupled with the adjacent AF material8 In recent years, this effect has been employed to stabilize the magnetization in spintronic devices, enhance the FMR frequency in microwave devices, and induce magnetoelectric coupling in multiferroic composites

Methods
Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call