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: Zr-Co-C (55 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-2107 Sc(Fe2Si)2 2 14 tetragonal P4_2/mnm [136] -0.493 . MP 0.56 0.51 . . . . . . DFT mp-1104929
MMD-2131 ScFeSi2 12 48 orthorhombic Pbam [55] -0.683 . MP 0.00 0.00 . . . . . . DFT mp-1199097
MMD-2217 Sc4FeSi7 1 12 orthorhombic Pmm2 [25] -0.453 . MP 0.09 0.06 . . . . . . DFT mp-1219407
MMD-2218 Sc2Fe3Si 4 24 orthorhombic Amm2 [38] -0.445 . MP 0.59 0.48 . . . . . . DFT mp-1219437
MMD-2220 Sc(Fe5Si)2 2 26 orthorhombic Immm [71] -0.256 . MP 1.54 1.46 . . . . . . DFT mp-1219497
MMD-2352 Sc2Fe3Si5 4 40 tetragonal P4/mnc [128] -0.692 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-21588
MMD-2359 ScFeSi 4 12 orthorhombic Pnma [62] -0.689 0 (stable) MP 0.01 0.01 . . . . . . DFT mp-22701
MMD-2369 ScFeSi2 24 96 orthorhombic Cmce [64] -0.681 . MP 0.16 0.13 . . . . . . DFT mp-30076
MMD-2374 Sc2FeSi2 4 20 monoclinic C2/m [12] -0.779 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-3618
MMD-2380 Sc3Fe2Si3 4 32 orthorhombic Cmcm [63] -0.756 0 (stable) MP 0.00 0.00 . . . . . . DFT mp-4755
MMD-2383 Sc(FeSi)2 4 20 orthorhombic Pbcm [57] -0.686 0 (stable) MP 0.20 0.18 . . . . . . DFT mp-505554
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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