Final Magnetic Moment0.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingNM |
Formation Energy / Atom1.882 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom1.882 eVThe energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures. |
Density2.70 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToO2 |
Band Gap0.000 eVIn general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic. |
Hermann MauguinFd3m [227] |
HallF 4d 2 3 1d |
Point Groupm3m |
Crystal Systemcubic |
Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)
A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Zn3CrS4 (mp-1080726) | 0.0175 | 0.324 | 3 |
Zn3CrSe4 (mp-1095028) | 0.0124 | 0.123 | 3 |
Zn3CrTe4 (mp-1087545) | 0.0105 | 0.115 | 3 |
CdSnSb2 (mp-10063) | 0.0250 | 0.000 | 3 |
GaCuS2 (mp-5238) | 0.0192 | 0.000 | 3 |
FeCu2GeS4 (mp-917359) | 0.0383 | 0.185 | 4 |
CoCu2GeS4 (mp-6498) | 0.0382 | 0.055 | 4 |
CoCu2GeS4 (mp-560428) | 0.0476 | 0.055 | 4 |
FeCu2GeS4 (mp-22053) | 0.0260 | 0.185 | 4 |
FeCu2GeSe4 (mp-1087471) | 0.0871 | 0.035 | 4 |
TiN (mp-998908) | 0.0000 | 0.301 | 2 |
VN (mp-1001826) | 0.0000 | 0.327 | 2 |
TaN (mp-1009833) | 0.0000 | 0.492 | 2 |
CuN (mp-13117) | 0.0000 | 0.784 | 2 |
HfC (mp-1002124) | 0.0000 | 0.641 | 2 |
Si (mp-149) | 0.0000 | 0.000 | 1 |
Sn (mp-117) | 0.0000 | 0.000 | 1 |
C (mp-66) | 0.0000 | 0.136 | 1 |
Ge (mp-32) | 0.0000 | 0.000 | 1 |
Se (mp-12771) | 0.0000 | 0.514 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: O |
Final Energy/Atom-3.0660 eV |
Corrected Energy-6.1321 eV
Uncorrected energy = -6.1321 eV
Corrected energy = -6.1321 eV
|
Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)