Crystal system |
tetragonal |
Space group number |
139 |
Hermann-Mauguin |
I4/mmm |
Hall |
-I 4 2 |
Point group |
4/mmm |
Normalized formula |
Co4N |
The number of formula units per unit cell |
2 |
The total number of atoms per unit cell |
10 |
The number of inequivalent sites per unit cell |
3 |
Structure search |
AGA search |
a (Å) |
3.7249 |
b (Å) |
3.7249 |
c (Å) |
7.3534 |
α (deg.) |
90.000 |
β (deg.) |
90.000 |
γ (deg.) |
90.000 |
Volume (Å3) |
102.026 |
Density (g/cm3) |
8.129 |
DFT calculations (details) | |
---|---|
Formation energy (vs. elemental phases) |
87.9 meV/atom |
Formation energy above hull |
87.9 meV/atom |
Compounds with the same formula: Co4N |
26 entries found |
Compounds with the same elements: Co-N |
183 entries found |
DFT calculations (details) | |
---|---|
Magnetic ordering |
Ferromagnetic |
Total magnetic moment |
12.29 μB/cell |
Averaged magnetic moment |
1.23 μB/atom |
Magnetic polarization, Js = μ0Ms |
1.40 T (= 1114.1 emu/cm3) |
LMTO-GF calculations (details) | |
---|---|
Curie temperature, TC |
|
DFT calculations (details) | |
---|---|
Magnetic anisotropy constant, Ka-c |
3.11 MJ/m3 (= 1.98 meV/cell) |
Magnetic easy axis |
c |
Magnetic hardness parameter, κ |
1.41 |
index | species | w | x | y | z | m (μB) | Esoc100 (meV) | Esoc001 (meV) |
---|---|---|---|---|---|---|---|---|
1 | N | 2a | 0.000000 | 0.000000 | 0.000000 | 0.09 | . | . |
2 | N | 2a | 0.500000 | 0.500000 | 0.500000 | 0.09 | . | . |
3 | Co | 4c | 0.000000 | 0.500000 | 0.000000 | 1.33 | . | . |
4 | Co | 4c | 0.500000 | 0.000000 | 0.000000 | 1.33 | . | . |
5 | Co | 4c | 0.500000 | 0.000000 | 0.500000 | 1.33 | . | . |
6 | Co | 4c | 0.000000 | 0.500000 | 0.500000 | 1.33 | . | . |
7 | Co | 4e | 0.000000 | 0.000000 | 0.254200 | 1.61 | . | . |
8 | Co | 4e | 0.000000 | 0.000000 | 0.745800 | 1.61 | . | . |
9 | Co | 4e | 0.500000 | 0.500000 | 0.754200 | 1.61 | . | . |
10 | Co | 4e | 0.500000 | 0.500000 | 0.245800 | 1.61 | . | . |
site i | site j | distance (Å) | Jij (meV) | ||||
---|---|---|---|---|---|---|---|
1 | N | 2a | 2 | N | 2a | 4.52 | . |
1 | N | 2a | 3 | Co | 4c | 1.86 | . |
1 | N | 2a | 4 | Co | 4c | 1.86 | . |
1 | N | 2a | 5 | Co | 4c | 4.12 | . |
1 | N | 2a | 6 | Co | 4c | 4.12 | . |
1 | N | 2a | 7 | Co | 4e | 1.87 | . |
1 | N | 2a | 8 | Co | 4e | 1.87 | . |
1 | N | 2a | 9 | Co | 4e | 3.19 | . |
1 | N | 2a | 10 | Co | 4e | 3.19 | . |
2 | N | 2a | 3 | Co | 4c | 4.12 | . |
2 | N | 2a | 4 | Co | 4c | 4.12 | . |
2 | N | 2a | 5 | Co | 4c | 1.86 | . |
2 | N | 2a | 6 | Co | 4c | 1.86 | . |
2 | N | 2a | 7 | Co | 4e | 3.19 | . |
2 | N | 2a | 8 | Co | 4e | 3.19 | . |
2 | N | 2a | 9 | Co | 4e | 1.87 | . |
2 | N | 2a | 10 | Co | 4e | 1.87 | . |
3 | Co | 4c | 4 | Co | 4c | 2.63 | . |
3 | Co | 4c | 5 | Co | 4c | 4.52 | . |
3 | Co | 4c | 6 | Co | 4c | 3.68 | . |
3 | Co | 4c | 7 | Co | 4e | 2.64 | . |
3 | Co | 4c | 8 | Co | 4e | 2.64 | . |
3 | Co | 4c | 9 | Co | 4e | 2.60 | . |
3 | Co | 4c | 10 | Co | 4e | 2.60 | . |
4 | Co | 4c | 5 | Co | 4c | 3.68 | . |
4 | Co | 4c | 6 | Co | 4c | 4.52 | . |
4 | Co | 4c | 7 | Co | 4e | 2.64 | . |
4 | Co | 4c | 8 | Co | 4e | 2.64 | . |
4 | Co | 4c | 9 | Co | 4e | 2.60 | . |
4 | Co | 4c | 10 | Co | 4e | 2.60 | . |
5 | Co | 4c | 6 | Co | 4c | 2.63 | . |
5 | Co | 4c | 7 | Co | 4e | 2.60 | . |
5 | Co | 4c | 8 | Co | 4e | 2.60 | . |
5 | Co | 4c | 9 | Co | 4e | 2.64 | . |
5 | Co | 4c | 10 | Co | 4e | 2.64 | . |
6 | Co | 4c | 7 | Co | 4e | 2.60 | . |
6 | Co | 4c | 8 | Co | 4e | 2.60 | . |
6 | Co | 4c | 9 | Co | 4e | 2.64 | . |
6 | Co | 4c | 10 | Co | 4e | 2.64 | . |
7 | Co | 4e | 8 | Co | 4e | 3.61 | . |
7 | Co | 4e | 9 | Co | 4e | 4.52 | . |
7 | Co | 4e | 10 | Co | 4e | 2.63 | . |
8 | Co | 4e | 9 | Co | 4e | 2.63 | . |
8 | Co | 4e | 10 | Co | 4e | 4.52 | . |
9 | Co | 4e | 10 | Co | 4e | 3.61 | . |
DFT calculations |
|
LMTO-GF calculations |
|
References |
Phys. Rev. B 94, 224424 (2016). DOI: 10.1103/PhysRevB.94.224424 |