Final Magnetic Moment0.001 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 / Atom0.040 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.168 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. |
Density2.31 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMg2Si + Si |
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 MauguinPm [6] |
HallP 2y |
Point Groupm |
Crystal Systemmonoclinic |
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 |
---|---|---|---|
Eu4O3F7 (mp-753354) | 0.6039 | 0.000 | 3 |
Y5Mg13Cu5 (mp-568046) | 0.5741 | 0.000 | 3 |
Na3InBi2 (mp-580161) | 0.5690 | 0.000 | 3 |
Mg2Co12As7 (mp-569003) | 0.6081 | 0.000 | 3 |
Y5Mg16Cu5 (mp-571074) | 0.6040 | 0.056 | 3 |
Er5Al3Ni3Ge4 (mp-638521) | 0.6257 | 0.000 | 4 |
K2BaCdSb2 (mp-863761) | 0.6539 | 0.000 | 4 |
K2SrCdSb2 (mp-863758) | 0.6732 | 0.000 | 4 |
Er4In(NiGe2)2 (mp-13508) | 0.7321 | 0.000 | 4 |
Tm4In(NiGe2)2 (mp-13511) | 0.7252 | 0.000 | 4 |
MgSi (mp-1073716) | 0.5241 | 0.181 | 2 |
Mg6Si5 (mp-1073935) | 0.4463 | 0.153 | 2 |
Mg5Si6 (mp-1075362) | 0.5689 | 0.200 | 2 |
Mg6Si5 (mp-1073910) | 0.5356 | 0.136 | 2 |
Mg6Si5 (mp-1073903) | 0.5413 | 0.149 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Si |
Final Energy/Atom-3.2957 eV |
Corrected Energy-71.7959 eV
Uncorrected energy = -72.5059 eV
Composition-based energy adjustment (0.071 eV/atom x 10.0 atoms) = 0.7100 eV
Corrected energy = -71.7959 eV
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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)