Determination of anisotropy constants via fitting of magnetic hysteresis to numerical calculation of Stoner–Wohlfarth model
Source abstract
Abstract
Anisotropy constants of magnetic materials are typically determined through angle-resolved Ferromagnetic Resonance (ar-FMR) and torque magnetometry, which can be time consuming measurements, thus limiting their utility. The Stoner–Wohlfarth model can be used to numerically fit measured magnetic hysteresis curves to more easily determine these anisotropy constants. To demonstrate this, 10 nm bct FexCoyMnz single-crystal films grown by molecular beam epitaxy on MgO(001) substrates were investigated. The hysteresis behavior measured by vibrating sample magnetometry was least-squares fit against numerically calculated hysteresis curves generated from the Stoner–Wohlfarth model to extract the anisotropy constants. The cubic anisotropy of different compositions of FeCoMn films was at ∼104 J/m3, which is on the same order of magnitude of bct Fe and Co thin films measured by ar-FMR and torque magnetometry techniques.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Magnetic properties of thin films · Magnetic Properties and Applications · Magnetic Properties of Alloys
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics, Montana State University , Bozeman, Montana 59717, USA
Funding
National Science Foundation
References (22)
Show source-provided references
1. Recent developments in perpendicular magnetic anisotropy thin films for data storage applications10.1016/j.vacuum.2017.01.031 ↗
2. Modeling and exploration of the voltage-controlled magnetic anisotropy effect for the next-generation low-power and high-speed MRAM applications10.1109/TNANO.2017.2660530 ↗
3. Giant magnetic anisotropy in tetragonal FeCo alloys10.1103/PhysRevLett.93.027203 ↗
4. Large moments in bcc FexCoyMnz ternary alloy thin films10.1063/1.5006347 ↗
5. Magnetic anisotropy in epitaxial metal films10.1016/0304-3991(92)90164-F ↗
6. A torque magnetometer for thin films applications10.1016/j.jmmm.2011.12.002 ↗
7. Combinatorial study of Fe-Co-V hard magnetic thin films10.1080/14686996.2017.1287520 ↗
8. Combinatorial exploration of rare-earth-free permanent magnets: Magnetic and microstructural properties of Fe-Co-W thin films10.1063/1.4775581 ↗
9. Combinatorial development of Fe–Co–Nb thin film magnetic nanocomposites10.1021/acscombsci.5b00116 ↗
10. Surface roughness and composition effects on the magnetic properties of electrodeposited Ni-Co alloys10.1016/0304-8853(95)01094-7 ↗
11. Effect of surface roughness on magnetic domain wall thickness, domain size and coercivity10.1063/1.1331065 ↗
12. On-the-fly machine-learning for high-throughput experiments: Search for rare-earth-free permanent magnets10.1038/srep06367 ↗
13. Machine learning autonomous identification of magnetic alloys beyond the Slater-Pauling limit10.1038/s43246-021-00135-0 ↗
14. Dependence of the magnetization and remanence of single-domain particles on the second cubic anisotropy constant10.1063/1.1415062 ↗
15. Influence of the cubic anisotropy constants on the hysteresis loops of single-domain particles: A Monte Carlo study10.1063/1.369539 ↗
16. Anisotropy and orientational dependence of magnetization reversal process in epitaxial ferromagnetic thin films10.1103/physrevb.51.15964 ↗
17. Theoretical hysteresis loops for single-domain particles with cubic anisotropy10.1016/s0304-8853(97)00180-7 ↗
18. Magnetization rotation in spin-valve multilayers10.1016/s0304-8853(97)00085-1 ↗
19. Magnetisation reversal by uniform rotation (Stoner–Wohlfarth model) in FCC cobalt nanoparticles10.1016/s0304-8853(01)01153-2 ↗
20. Properties of Fe single-crystal films grown on (100)GaAs by molecular-beam epitaxy10.1063/1.337886 ↗
21. FMR of cubic cobalt grown by molecular beam epitaxy on GaAs10.1063/1.334984 ↗
22. Structure induced magnetic anisotropy behavior in Co/GaAs(001) films10.1063/1.353531 ↗