Final Magnetic Moment0.012 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-0.772 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. |
Density9.84 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*
|
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 |
---|---|---|---|
CeInPt (mp-640922) | 0.0489 | 0.000 | 3 |
HoInCu (mp-3015) | 0.0586 | 0.000 | 3 |
CeInIr (mp-20449) | 0.0456 | 0.000 | 3 |
NdSnPd (mp-22419) | 0.0374 | 0.000 | 3 |
TbInCu (mp-19782) | 0.0379 | 0.000 | 3 |
Tb3Mn3Ga2Si (mp-22582) | 0.6182 | 0.341 | 4 |
Lu3Mn3Ga2Si (mp-568631) | 0.6105 | 0.072 | 4 |
Tm3Mn3Ga2Si (mp-570450) | 0.5904 | 0.090 | 4 |
Dy3Mn3Ga2Si (mp-21038) | 0.5970 | 0.322 | 4 |
U3Al3NiRu2 (mp-1080528) | 0.4453 | 0.087 | 4 |
USe2 (mp-8591) | 0.2092 | 0.032 | 2 |
Mn2P (mp-571176) | 0.2617 | 0.000 | 2 |
Ti2P (mp-30218) | 0.0753 | 0.000 | 2 |
CeSe2 (mp-1021484) | 0.2252 | 0.019 | 2 |
US2 (mp-2849) | 0.1377 | 0.091 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: La Pd Pb_d |
Final Energy/Atom-5.3799 eV |
Corrected Energy-48.4190 eV
Uncorrected energy = -48.4190 eV
Corrected energy = -48.4190 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)