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 / Atom-0.917 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 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. |
Density9.61 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
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 MauguinP62m [189] |
HallP 6 2 |
Point Group6m2 |
Crystal Systemhexagonal |
Topological ClassificationTI*
|
SubclassificationSEBR†
|
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 |
---|---|---|---|
SmAlCu (mp-979972) | 0.0339 | 0.000 | 3 |
GdAlPd (mp-20058) | 0.0655 | 0.000 | 3 |
ThAlPd (mp-1078527) | 0.0632 | 0.000 | 3 |
TbAlCu (mp-1079357) | 0.0597 | 0.000 | 3 |
NdAlCu (mp-1080560) | 0.0474 | 0.000 | 3 |
Yb3In3Ge2Au (mp-981207) | 0.4155 | 0.000 | 4 |
Lu3Mn3Ga2Si (mp-568631) | 0.4152 | 0.072 | 4 |
Y3Al3NiGe2 (mp-10209) | 0.4415 | 0.000 | 4 |
Er3Al3NiGe2 (mp-12388) | 0.4303 | 0.000 | 4 |
U3Al3NiRu2 (mp-1080528) | 0.0908 | 0.087 | 4 |
Fe2P (mp-778) | 0.3713 | 0.000 | 2 |
Pu2Co (mp-20026) | 0.4328 | 0.060 | 2 |
BaI2 (mp-568536) | 0.3644 | 0.006 | 2 |
BaCl2 (mp-567680) | 0.3555 | 0.030 | 2 |
Co2As (mp-1079254) | 0.4395 | 0.071 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Th Al Rh_pv |
Final Energy/Atom-7.0829 eV |
Corrected Energy-63.7462 eV
Uncorrected energy = -63.7462 eV
Corrected energy = -63.7462 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)