Determining the coercivity of anisotropic Heisenberg magnets by Monte Carlo sampling: Application to the design of permanent magnets
Source abstract
Abstract
Abstract Monte Carlo methods are widely used to study magnetism. However, their use to the calculation of coercivity has been problematic because of difficulties in quantifying Monte Carlo time. Here we propose a new approach of studying coercivity based on Monte Carlo sampling of the switching time at different reverse fields. This method allows comparative analysis of how coercivity is affected by various factors without needing time quantification of the Monte Carlo step. We apply the new method to study antiferromagnet-ferromagnet exchange coupling systems and show that practically large coercivity and enhanced maximum energy product can be achieved by properly adding antiferromagnet to high-magnetization ferromagnets such as Fe16N2. The finding is important to the design of new rare-earth-free permanent magnets.
Source: openaire · Quality: candidate unverified · Source record ↗
Research context
OpenAlex topics: Magnetic properties of thin films · Magnetic and transport properties of perovskites and related materials · Magnetic Properties of Alloys
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (28)
Show source-provided references
1. Geyer · Introduction to Markov Chain Monte Carlo · 2011
2. Magnetization switching in a heisenberg model for small ferromagnetic particles10.1103/PhysRevB.58.265 ↗
3. Modeling of hysteresis loops by Monte Carlo simulation10.1063/1.4938549 ↗
4. Monte Carlo simulation with time step quantification in terms of langevin dynamics10.1103/PhysRevLett.84.163 ↗
5. Real time quantification of monte carlo steps for different time scales10.1063/1.373163 ↗
6. O. Chubykalo, J. Kauffman, B. Lengsfield, R. Smirnov-Rueda, Long-time calculation of the thermal magnetization reversal using metropolis monte carlo, J. Magn. Magn. Mater. 242–245 (2002) 1052–1056, proceedings of the Joint European Magnetic Symposia (JEMS’01). doi:10.1016/S0304-8853(01)01355-5. http://www.sciencedirect.com/science/article/pii/S0304885301013555.10.1016/S0304-8853(01)01355-5 ↗
7. Monte carlo technique with a quantified time step: Application to the motion of magnetic moments10.1103/PhysRevB.67.064422 ↗
8. Mapping the monte carlo scheme to langevin dynamics: A fokker-planck approach10.1103/PhysRevLett.96.067208 ↗
9. Time-quantified monte carlo algorithm for interacting spin array micromagnetic dynamics10.1103/PhysRevB.73.224438 ↗
10. Distributions of switching times of single-domain particles using a time quantified monte carlo method10.1016/j.jmmm.2007.03.195 ↗
11. Permanent magnet design assisted by antiferromagnet-ferromagnet interface coupling: A Monte Carlo study10.1016/j.jmmm.2019.166360 ↗
12. Current progress and future challenges in rare-earth-free permanent magnets10.1016/j.actamat.2018.07.049 ↗
13. Environment-friendly bulk Fe16n2 permanent magnet: Review and prospective10.1016/j.jmmm.2019.165962 ↗
14. New magnetic material having ultrahigh magnetic moment10.1063/1.1654030 ↗
15. Fabrication of Fe16N2 films by sputtering process and experimental investigation of origin of giant saturation magnetization in Fe16N210.1109/TMAG.2011.2170156 ↗
16. J.-P. Wang, Y. Jiang, M.A. Mehedi, J. Liu, Y. Wu, B. Ma, Fe16N2: From a 40-year mystery of magnetic materials to one of promises for rare-earth-free magnets (invited talk), in: Intermag, vol. EA-02, 2018.10.1109/INTMAG.2018.8508460 ↗
17. Perpendicular magnetic anisotropy and high spin-polarization ratio in epitaxial Fe-N thin films10.1103/PhysRevB.84.245310 ↗
18. T. Ogawa, Y. Ogata, R. Gallage, N. Kobayashi, N. Hayashi, Y. Kusano, S. Yamamoto, K. Kohara, M. Doi, M. Takano, M. Takahashi, Challenge to the synthesis of α′′-Fe16N2 compound nanoparticle with high saturation magnetization for rare earth free new permanent magnetic material, Appl. Phys. Express 6 (7) (2013) 073007. doi:10.7567/apex.6.073007. https://doi.org/10.7567%2Fapex.6.073007.10.7567/APEX.6.073007 ↗
19. Epitaxial Fe16N2 thin film on nonmagnetic seed layer10.1063/1.5028396 ↗
20. Heavy-metal-free, low-damping, and non-interface perpendicular Fe16N2 thin film and magnetoresistance device10.1002/pssr.201900089 ↗
21. Y. Jiang, M.A. Mehedi, E. Fu, Y. Wang, L.F. Allard, J.-P. Wang, Synthesis of Fe16N2 compound free-standing foils with 20 MGOe magnetic energy product by nitrogen ion-implantation, Sci. Rep. 6 (2016) 25436 EP –, article. doi: 10.1038/srep25436.10.1038/srep25436 ↗
22. Synthesis of α″-Fe16N2 compound anisotropic magnet by the strained-wire method
23. Facile synthesis of single-phase spherical α′′-Fe16N2/Al2O3 core-shell nanoparticles via a gas-phase method10.1063/1.4798959 ↗
24. New magnetic anisotropy10.1103/PhysRev.105.904 ↗
25. Exchange bias10.1016/S0304-8853(98)00266-2 ↗
26. Consequences of spin-flop coupling in exchange biased films10.1103/PhysRevLett.81.4516 ↗
27. Coercivity enhancement in exchange biased systems driven by interfacial magnetic frustration10.1103/PhysRevLett.84.3466 ↗
28. Equation of state calculations by fast computing machines10.1063/1.1699114 ↗