Additionally, there are concerns about losing control over proprietary specifications and end-user information. Since HRE-free Neodymium magnets fall outside the export control list, they have regained attention as a viable alternative.
Based on atomic number and properties, REEs are divided into 2 or 3 subgroups. In a 3-subgroup system, La, Ce, Pr, and Nd are light rare earths; Sm, Eu, and Gd are medium rare earths; and Tb, Dy, Ho, Er, Tm, Yb, and Lu are heavy rare earths. In a 2-subgroup system, La to Eu (7 elements) are light rare earths (LREEs), and Gd to Lu (7 elements) are heavy rare earths (HREEs). LREEs are generally more abundant and easier to extract from common deposits, while HREEs are rarer and more expensive to extract than LREEs.
The necessary intrinsic magnetic properties for any permanent magnet are a high Curie temperature (Tc), high saturation magnetization (Ms), and high anisotropy field (HA). HA is the primary source of intrinsic coercivity in rare earth magnets, as it determines how strongly the magnetic moments are aligned along preferred crystallographic directions.
The Nd2Fe14B compound stands out by combining high Ms with sufficient Tc and HA, enabling exceptional energy density and practical advantages like cost-effectiveness and processability. This has allowed Neodymium magnets to commercialize widely and revolutionize industries since the 1980s.
In practical applications, coercivity is pivotal, as it governs the magnet’s resistance to demagnetization from external fields or heat, and thus its thermal stability—directly influencing application potential in high-stress environments.
Compounds like Tb2Fe14B and Dy2Fe14B exhibit low Ms but exceptionally high HA, making them ideal for boosting coercivity. By partially replacing Nd with Dy or Tb in the Nd2Fe14B lattice, HA increases, which elevates coercivity while maintaining acceptable Ms. This substitution strengthens the magnetocrystalline anisotropy, stabilizing domains against thermal fluctuations and demagnetizing fields.
HREEs are not essential for all Neodymium magnets but are added to enhance intrinsic coercivity. Without HREEs, standard Neodymium magnets can lose magnetism under heat or strong opposing fields, limiting their use in high-performance scenarios. HREEs are integrated during the manufacturing process of Neodymium magnets.
The earliest alloying process involves adding a certain proportion of Dy and Tb to the raw materials, then through melting to homogenize all elements, forming (HRE, Nd)2Fe14B phase with high magnetocrystalline anisotropy field to achieve coercivity improvement. However, as heavy rare earths are critical materials prone to supply chain disruptions and price volatility, Neodymium magnets produced this way face increased costs and raw material challenges. Additionally, due to antiferromagnetic coupling between heavy rare earth elements and Fe, remanence and maximum energy product are significantly reduced.
Therefore, reducing heavy rare earth usage while ensuring Neodymium magnets obtain high coercivity has been a focus for industry and academia, leading to processes like HRE-less (HRE-lean) and HRE-free Neodymium magnets.
Grain boundary doping technology mixes HREE-containing dopants with the original magnetic powder during the powder preparation process. The core of grain boundary doping is not changing the main phase structure of the magnet; heavy rare earth elements diffuse from grain boundaries into main phase grains during sintering, forming a magnetic hardening layer in the boundary region, optimizing grain boundary phase and interface structure, enhancing demagnetization decoupling effect, thus improving coercivity.
Grain boundary diffusion (GBD) process performs heavy rare earth elements diffusion on sintered Neodymium magnet blanks. At diffusion temperature, heavy rare earth elements diffuse along grain boundaries into the magnet, replacing part of Nd at grain boundaries and forming (HRE, Nd)2Fe14B core-shell structure around main phase grains, with HREE attaching to grain corner regions, enhancing the anisotropy field of the main phase, making demagnetization decoupling more pronounced. The most notable feature of GBD process is increasing coercivity while maintaining high remanence, and it has become the mainstream process.