Final Magnetic Moment0.005 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-1.073 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. |
Density12.75 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 ClassificationSM*
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SubclassificationESFD†
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Crossing TypePoint
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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 |
---|---|---|---|
MnGePd (mp-610972) | 0.1007 | 0.045 | 3 |
TbInAu (mp-22718) | 0.0967 | 0.000 | 3 |
YbInPt (mp-1078378) | 0.0805 | 0.000 | 3 |
HoSnIr (mp-1079423) | 0.0925 | 0.000 | 3 |
TmSnPt (mp-1080806) | 0.1009 | 0.000 | 3 |
Mg3Al9FeSi5 (mp-7062) | 0.6551 | 0.006 | 4 |
Mg3Al8FeSi6 (mp-571315) | 0.7203 | 0.141 | 4 |
U3Al3NiRu2 (mp-1080528) | 0.6911 | 0.088 | 4 |
SiPd2 (mp-697068) | 0.2184 | 0.000 | 2 |
USe2 (mp-8591) | 0.1417 | 0.032 | 2 |
Mn2P (mp-571176) | 0.2295 | 0.000 | 2 |
Mn2P (mp-1849) | 0.2211 | 0.000 | 2 |
GePd2 (mp-423) | 0.2273 | 0.000 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Lu_3 Sn_d Pt |
Final Energy/Atom-5.9404 eV |
Corrected Energy-53.4639 eV
-53.4639 eV = -53.4639 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)