Database statistics:

A total of 3,826 entries, including 300+ Fe-based rare-earth-free magnets discovered through our adaptive genetic algorithm (AGA) searches, are registered in our database. Data statistics are summarized here.

Phase diagrams:

Binary phases: Fe-N (38 entries), Fe-S (45 entries), Fe-Si (47 entries), Co-N (183 entries), Zr-Co (42 entries), among others.
Ternary phases: Fe-Co-N (272 entries), Fe-Co-S (34 entries), Zr-Co-B (50 entries), Zr-Co-C (55 entries), Zr-Co-N (79 entries), among others.

Benchmark test:

Benchmark results are summarized here, where we compare theoretical and experimental values.
random selection: Co-B (6 entries found)
Displaying 11 entries out of 11 entries found.
Crystallographic data Sstructural stability [Footnotes] Magnetic properties [Footnotes, magnetic units] Methods References
Materials ID Formula Formula units per cell Atomic sites per cell Crystal system Space group [Number] Formation energy (eV/atom) Energy relative to convex hull (eV/atom) Structure search Averaged magnetic moment (μB/atom) Magnetic polarization, Js (T) Magnetic easy axis Magnetic anisotropy constants:
Ka-c, Kb-c, Kb-a, Kd-a (MJ/m3)		 Curie temperature, TC (K) Methods References
MMD-42 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.018 0.071 AGA search 1.57 1.74 c 0.90 1.09 0.18 . . DFT DOI link
MMD-43 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.014 0.076 AGA search 1.61 1.78 c 1.65 1.48 -0.17 . . DFT DOI link
MMD-44 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.014 0.076 AGA search 1.60 1.77 c 0.88 1.05 0.17 . . DFT DOI link
MMD-359 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.018 0.071 AGA search 1.57 1.74 c 0.90 1.09 0.18 . . DFT MS
MMD-436 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.018 0.071 AGA search 1.57 1.74 c 0.90 1.08 0.18 . . DFT MS
MMD-437 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.017 0.073 AGA search 1.63 1.79 c 0.66 0.74 0.08 . . DFT MS
MMD-438 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.017 0.073 AGA search 1.60 1.76 c 0.81 1.07 0.26 . . DFT MS
MMD-439 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.014 0.076 AGA search 1.61 1.78 c 1.65 1.48 -0.17 . . DFT MS
MMD-440 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.013 0.076 AGA search 1.63 1.79 c 0.49 0.94 0.44 . . DFT MS
MMD-441 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.012 0.078 AGA search 1.61 1.78 c 1.46 1.40 -0.06 . . DFT MS
MMD-442 Fe3Co2N 4 24 orthorhombic Amm2 [38] -0.011 0.079 AGA search 1.63 1.80 c 1.15 1.12 -0.03 . . DFT MS
Footnotes:
  1. Formation energy:
    We perform DFT calculations to calculate the total enegies of all the structures. The formation energy is computed with respect to a linear combination of the total energies of reference elemental phases. When the formation energies are plotted as a function of chemical composition, a set of stable compounds forms a convex hull, which represents a boundary (theoretical lower limit) in a compositional phase diagram. Metastable compounds lie above the hull, and the energy relative to the hull (distance to the hull) is a useful quantity to examine the metastability of a new compound. The lower the formation energy above the convex hull, the more likely it is for the material to exist.
  2. Magnetic anisotropy constants:
    Magnetic anisotropy constant, Ka-c, is defined as Ka-c = Ea-Ec, where Ea and Ec are the total energies per volume for the magnetization oriented along the crystallographic a and c axes, respectively. Similarly, Kb-c and Kb-a are defined as Kb-c = Eb-Ec and Kb-a = Eb-Ea, respectively. For cubic crystal systems, magnetic anisotropy constant is calculated as Kd-a = Ed-Ea, where Ed is the total energy per volume for the magnetization oriented along the body-diagonal direction of the unit cell.
Collaborative PIs:
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