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-0.119 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.021 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. |
Density4.93 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMg2Sn + Sn |
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 MauguinP4/mmm [123] |
Hall-P 4 2 |
Point Group4/mmm |
Crystal Systemtetragonal |
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 |
---|---|---|---|
InCuPt2 (mp-639659) | 0.0617 | 0.000 | 3 |
TiAgHg2 (mp-30341) | 0.1249 | 0.141 | 3 |
MnGaNi2 (mp-1066921) | 0.0276 | 0.028 | 3 |
FeNiPt2 (mp-13463) | 0.1591 | 0.000 | 3 |
TiCdHg2 (mp-11300) | 0.0361 | 0.089 | 3 |
Cr8Ni50Mo15W2 (mp-767372) | 0.3133 | 0.028 | 4 |
CrFeCoNi (mp-1012640) | 0.3329 | 0.065 | 4 |
CrFeCoNi (mp-1096923) | 0.3817 | 0.193 | 4 |
Rb3In (mp-974982) | 0.0166 | 0.160 | 2 |
Rb3Mn (mp-974970) | 0.0002 | 0.689 | 2 |
HgPt (mp-623) | 0.0028 | 0.116 | 2 |
ThH3 (mp-861653) | 0.0055 | 0.049 | 2 |
LiMg3 (mp-1094567) | 0.0082 | 0.028 | 2 |
K (mp-972981) | 0.2128 | 0.008 | 1 |
Pr (mp-567630) | 0.2388 | 0.008 | 1 |
Sc (mp-1055932) | 0.2659 | 0.052 | 1 |
Ca (mp-45) | 0.2288 | 0.000 | 1 |
Pr (mp-1059528) | 0.2714 | 0.010 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Sn_d |
Final Energy/Atom-2.9242 eV |
Corrected Energy-5.8483 eV
-5.8483 eV = -5.8483 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)