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-0.396 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. |
Density6.81 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 MauguinC2/m [12] |
Hall-C 2y |
Point Group2/m |
Crystal Systemmonoclinic |
Topological ClassificationTI*
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SubclassificationSEBR†
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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 |
---|---|---|---|
NbPSe (mp-7524) | 0.6097 | 0.061 | 3 |
Er2Ge5Rh3 (mp-984743) | 0.6303 | 0.000 | 3 |
Ho2Ge5Rh3 (mp-17534) | 0.6067 | 0.000 | 3 |
YbFeGe (mp-628705) | 0.6121 | 0.144 | 3 |
Dy2Ge5Rh3 (mp-866028) | 0.6096 | 0.000 | 3 |
NbAs2 (mp-7598) | 0.2352 | 0.000 | 2 |
TaSb2 (mp-11697) | 0.2306 | 0.000 | 2 |
CrAs2 (mp-15681) | 0.1373 | 0.006 | 2 |
NbSb2 (mp-1969) | 0.1417 | 0.000 | 2 |
As2W (mp-1077179) | 0.2351 | 0.003 | 2 |
Rb (mp-640416) | 0.7315 | 0.057 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: V_pv As |
Final Energy/Atom-6.5304 eV |
Corrected Energy-39.1823 eV
-39.1823 eV = -39.1823 eV (uncorrected energy)
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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)