Final Magnetic Moment0.564 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-0.161 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. |
Density2.38 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 MauguinI43d [220] |
HallI 4bd 2c 3 |
Point Group43m |
Crystal Systemcubic |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
TePb (mp-19717) | <1 0 0> | <1 0 0> | 173.5 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 173.5 |
CdTe (mp-406) | <1 0 0> | <1 0 0> | 173.5 |
TiO2 (mp-2657) | <0 0 1> | <1 0 0> | 173.5 |
InSb (mp-20012) | <1 0 0> | <1 0 0> | 173.5 |
Au (mp-81) | <1 0 0> | <1 0 0> | 173.5 |
SiC (mp-8062) | <1 0 0> | <1 0 0> | 173.5 |
MgF2 (mp-1249) | <1 0 0> | <1 0 0> | 173.5 |
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 |
---|---|---|---|
Li12Mg3Si4 (mp-8331) | 0.2490 | 0.009 | 3 |
Li12Al3Si4 (mp-14378) | 0.3328 | 0.094 | 3 |
NiGePt2 (mp-29752) | 0.7152 | 0.000 | 3 |
Li15Ge4 (mp-1777) | 0.1124 | 0.000 | 2 |
Na15Pb4 (mp-21895) | 0.0833 | 0.000 | 2 |
Li15Au4 (mp-567395) | 0.3088 | 0.000 | 2 |
Th4H15 (mp-24202) | 0.3342 | 0.000 | 2 |
Li15Si4 (mp-569849) | 0.0884 | 0.003 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Na_pv Sn_d |
Final Energy/Atom-2.0379 eV |
Corrected Energy-77.4415 eV
-77.4415 eV = -77.4415 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)