Crystal system |
orthorhombic |
Space group number |
25 |
Hermann-Mauguin |
Pmm2 |
Hall |
P 2 -2 |
Point group |
mm2 |
Normalized formula |
Ti2CuNi |
The number of formula units per unit cell |
1 |
The total number of atoms per unit cell |
4 |
The number of inequivalent sites per unit cell |
4 |
Structure search |
MP |
a (Å) |
2.8737 |
b (Å) |
4.2511 |
c (Å) |
4.5226 |
α (deg.) |
90.000 |
β (deg.) |
90.000 |
γ (deg.) |
90.000 |
Volume (Å3) |
55.250 |
Density (g/cm3) |
6.551 |
DFT calculations (details) | |
---|---|
Formation energy (vs. elemental phases) |
-219.3 meV/atom |
Formation energy above hull |
|
Compounds with the same formula: Ti2CuNi |
2 entries found |
Compounds with the same elements: Ti-Cu-Ni |
6 entries found |
Binary compounds in Ti-Cu system |
No entries found |
Binary compounds in Ti-Ni system |
16 entries found |
Binary compounds in Cu-Ni system |
6 entries found |
DFT calculations (details) | |
---|---|
Magnetic ordering |
Ferromagnetic |
Total magnetic moment |
0.02 μB/cell |
Averaged magnetic moment |
0.01 μB/atom |
Magnetic polarization, Js = μ0Ms |
0.00 T (= 0.0 emu/cm3) |
LMTO-GF calculations (details) | |
---|---|
Curie temperature, TC |
|
DFT calculations (details) | |
---|---|
Magnetic easy axis |
|
Magnetic hardness parameter, κ |
|
index | species | w | x | y | z | m (μB) | Esoc100 (meV) | Esoc001 (meV) |
---|---|---|---|---|---|---|---|---|
1 | Ti | 1c | 0.500000 | 0.000000 | 0.221053 | 0.01 | . | . |
2 | Ti | 1d | 0.500000 | 0.500000 | 0.779342 | -0.00 | . | . |
3 | Cu | 1b | 0.000000 | 0.500000 | 0.310098 | 0.00 | . | . |
4 | Ni | 1a | 0.000000 | 0.000000 | 0.689507 | 0.00 | . | . |
site i | site j | distance (Å) | Jij (meV) | ||||
---|---|---|---|---|---|---|---|
1 | Ti | 1c | 2 | Ti | 1d | 2.92 | . |
1 | Ti | 1c | 3 | Cu | 1b | 2.60 | . |
1 | Ti | 1c | 4 | Ni | 1a | 2.56 | . |
2 | Ti | 1d | 3 | Cu | 1b | 2.56 | . |
2 | Ti | 1d | 4 | Ni | 1a | 2.60 | . |
3 | Cu | 1b | 4 | Ni | 1a | 2.73 | . |
DFT calculations |
|
LMTO-GF calculations |
|
References |
Materials Project: mp-1217130 |