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 / Atom0.000 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom< 0.001 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. |
Density3.51 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToBa |
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 MauguinCmcm [63] |
Hall-C 2c 2 |
Point Groupmmm |
Crystal Systemorthorhombic |
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 |
---|---|---|---|
NaLi5N2 (mp-29929) | 0.4445 | 0.248 | 3 |
MnIn2W (mp-632623) | 0.4096 | 0.703 | 3 |
ThInAg2 (mp-862932) | 0.3790 | 0.000 | 3 |
GdCdPd2 (mp-866034) | 0.4403 | 0.032 | 3 |
UAl2Cu (mp-1064586) | 0.4393 | 0.474 | 3 |
VFeCoGe (mp-1063914) | 0.4927 | 0.000 | 4 |
TiGaFeCo (mp-998964) | 0.4927 | 0.000 | 4 |
TiFeCoSb (mp-998973) | 0.4927 | 0.186 | 4 |
TiFeCoSi (mp-998971) | 0.4927 | 0.029 | 4 |
TiAlFeCo (mp-998980) | 0.4927 | 0.000 | 4 |
YbGa (mp-396) | 0.1528 | 0.000 | 2 |
CeCd (mp-11291) | 0.0437 | 0.073 | 2 |
MnNi (mp-1797) | 0.1247 | 0.037 | 2 |
LaMg3 (mp-1094174) | 0.0487 | 0.001 | 2 |
CaMg (mp-1094998) | 0.1102 | 0.001 | 2 |
Cu (mp-1010136) | 0.2080 | 0.036 | 1 |
Mg (mp-1056351) | 0.2669 | 0.029 | 1 |
Sc (mp-10641) | 0.1178 | 0.102 | 1 |
Ca (mp-166) | 0.2245 | 0.021 | 1 |
Ca (mp-21) | 0.1032 | 0.024 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv |
Final Energy/Atom-1.9189 eV |
Corrected Energy-3.8378 eV
-3.8378 eV = -3.8378 eV (uncorrected energy)
|
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)