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: Nb-Cr (11 entries found)
Displaying 12 entries out of 12 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-3140 Sc3Si3Ni2 4 32 orthorhombic Cmcm [63] -0.884 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-11338
MMD-3259 Sc4Si7Ni 1 12 orthorhombic Pmm2 [25] -0.482 . MP 0.00 0.00 . . . . . . DFT mp-1219409
MMD-3444 Sc3(Si2Ni)2 4 36 orthorhombic Pnma [62] -0.846 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-542486
MMD-3447 Sc4Si7Ni12 6 138 orthorhombic Immm [71] -0.723 . MP 0.00 0.00 . . . . . . DFT mp-567443
MMD-3452 Sc6Si11Ni18 4 140 orthorhombic Immm [71] -0.767 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-570147
MMD-3439 Sc6Si7Ni16 4 116 cubic Fm-3m [225] -0.766 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-5382
MMD-3390 Sc3Si4Ni11 2 36 hexagonal P6_3/mmc [194] -0.610 . MP 0.00 0.00 . . . . . . DFT mp-27918
MMD-3412 Sc(SiNi)2 2 10 tetragonal I4/mmm [139] -0.796 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-3587
MMD-3365 ScSi3Ni2 4 24 tetragonal I4/mmm [139] -0.671 . MP 0.00 0.00 . . . . . . DFT mp-15605
MMD-3385 ScSiNi 4 12 orthorhombic Pnma [62] -0.895 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-22426
MMD-3409 ScSi3Ni 4 20 orthorhombic Cmmm [65] -0.627 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-3129
MMD-3492 Sc3Si3Ni 4 28 monoclinic C2/m [12] -0.867 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-8392
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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