Final Magnetic Moment0.775 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingUnknown |
Formation Energy / Atom-0.513 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom1.550 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. |
Density4.24 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToY2S3 + S |
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%)
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| substrate material | substrate orientation | film orientation | MCIA† [Å2] |
|---|---|---|---|
| AlN (mp-661) | <0 0 1> | <1 0 0> | 306.5 |
| CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 61.3 |
| CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 86.7 |
| GaAs (mp-2534) | <1 0 0> | <1 0 0> | 306.5 |
| BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 306.5 |
| DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 61.3 |
| LaAlO3 (mp-2920) | <0 0 1> | <1 0 0> | 306.5 |
| LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 306.5 |
| LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 260.1 |
| CeO2 (mp-20194) | <1 1 1> | <1 0 0> | 306.5 |
| KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 183.9 |
| CdS (mp-672) | <0 0 1> | <1 1 1> | 106.2 |
| CdS (mp-672) | <1 0 0> | <1 0 0> | 306.5 |
| CdS (mp-672) | <1 1 1> | <1 1 0> | 260.1 |
| LiF (mp-1138) | <1 0 0> | <1 0 0> | 306.5 |
| TePb (mp-19717) | <1 1 0> | <1 1 0> | 173.4 |
| Ag (mp-124) | <1 0 0> | <1 0 0> | 306.5 |
| BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 173.4 |
| KCl (mp-23193) | <1 1 0> | <1 1 0> | 173.4 |
| DyScO3 (mp-31120) | <0 1 0> | <1 1 0> | 86.7 |
| DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 183.9 |
| InAs (mp-20305) | <1 0 0> | <1 0 0> | 306.5 |
| BN (mp-984) | <0 0 1> | <1 0 0> | 306.5 |
| BN (mp-984) | <1 0 0> | <1 1 0> | 173.4 |
| BN (mp-984) | <1 1 1> | <1 0 0> | 245.2 |
| MoS2 (mp-1434) | <0 0 1> | <1 1 1> | 106.2 |
| CdTe (mp-406) | <1 1 0> | <1 1 0> | 260.1 |
| ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 306.5 |
| KTaO3 (mp-3614) | <1 0 0> | <1 1 0> | 260.1 |
| LiF (mp-1138) | <1 1 0> | <1 1 0> | 260.1 |
| Bi2Te3 (mp-34202) | <0 0 1> | <1 0 0> | 306.5 |
| SiC (mp-7631) | <1 0 1> | <1 0 0> | 245.2 |
| Fe3O4 (mp-19306) | <1 0 0> | <1 0 0> | 306.5 |
| TiO2 (mp-2657) | <1 0 1> | <1 1 0> | 260.1 |
| GaSe (mp-1943) | <0 0 1> | <1 0 0> | 306.5 |
| BN (mp-984) | <1 1 0> | <1 1 0> | 173.4 |
| Bi2Se3 (mp-541837) | <0 0 1> | <1 1 1> | 106.2 |
| GdScO3 (mp-5690) | <0 0 1> | <1 1 0> | 260.1 |
| GdScO3 (mp-5690) | <0 1 0> | <1 1 0> | 86.7 |
| GdScO3 (mp-5690) | <1 0 0> | <1 0 0> | 183.9 |
| LiGaO2 (mp-5854) | <1 0 1> | <1 0 0> | 183.9 |
| TeO2 (mp-2125) | <0 0 1> | <1 1 0> | 260.1 |
| TeO2 (mp-2125) | <0 1 1> | <1 0 0> | 306.5 |
| TbScO3 (mp-31119) | <0 0 1> | <1 1 0> | 260.1 |
| TbScO3 (mp-31119) | <1 0 0> | <1 0 0> | 183.9 |
| PbSe (mp-2201) | <1 0 0> | <1 0 0> | 306.5 |
| BaTiO3 (mp-5986) | <1 0 1> | <1 0 0> | 183.9 |
| MgO (mp-1265) | <1 0 0> | <1 0 0> | 306.5 |
| GdScO3 (mp-5690) | <1 1 0> | <1 0 0> | 61.3 |
| Mg (mp-153) | <1 0 0> | <1 0 0> | 245.2 |
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 |
|---|---|---|---|
| HfNi2 (mp-30708) | 0.0000 | 0.046 | 2 |
| LaRu2 (mp-2019) | 0.0000 | 0.000 | 2 |
| LuIr2 (mp-1761) | 0.0000 | 0.000 | 2 |
| EuAl2 (mp-20111) | 0.0000 | 0.000 | 2 |
| ErCo2 (mp-537) | 0.0000 | 0.000 | 2 |
| ScNi4Sn (mp-11808) | 0.0013 | 0.000 | 3 |
| ZrInNi4 (mp-637771) | 0.0009 | 0.005 | 3 |
| ScInCu4 (mp-13240) | 0.0046 | 0.000 | 3 |
| YbNi4Au (mp-1024977) | 0.0002 | 0.040 | 3 |
| TmInCu4 (mp-1024957) | 0.0015 | 0.000 | 3 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-points28 |
U Values-- |
PseudopotentialsVASP PAW: S Y_sv |
Final Energy/Atom-4.9783 eV |
Corrected Energy-32.5236 eV
-32.5236 eV = -29.8697 eV (uncorrected energy) - 2.6538 eV (MP Anion Correction)
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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)