Final Magnetic Moment0.006 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 / Atom0.026 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.153 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. |
Density2.29 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 MauguinP1 [1] |
HallP 1 |
Point Group1 |
Crystal Systemtriclinic |
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 |
---|---|---|---|
Na3InBi2 (mp-580161) | 0.4921 | 0.000 | 3 |
CeAlRu (mp-604008) | 0.5522 | 0.000 | 3 |
LaZnRh (mp-570525) | 0.5622 | 0.000 | 3 |
CeAlRh (mp-3344) | 0.5396 | 0.000 | 3 |
HfGePd (mp-17746) | 0.5558 | 0.000 | 3 |
Yb3In3Ge2Au (mp-981207) | 0.6549 | 0.000 | 4 |
Er5Al3Ni3Ge4 (mp-638521) | 0.4162 | 0.000 | 4 |
K2BaCdSb2 (mp-863761) | 0.6362 | 0.000 | 4 |
K2SrCdSb2 (mp-863758) | 0.6555 | 0.000 | 4 |
Mg3Al8FeSi6 (mp-571315) | 0.6882 | 0.141 | 4 |
Mg6Si5 (mp-1073911) | 0.4463 | 0.168 | 2 |
Mg6Si5 (mp-1073921) | 0.5567 | 0.131 | 2 |
Mg5Si6 (mp-1075433) | 0.5602 | 0.196 | 2 |
Mg6Si5 (mp-1073910) | 0.4583 | 0.136 | 2 |
Mg6Si5 (mp-1073903) | 0.5319 | 0.149 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Si |
Final Energy/Atom-3.3104 eV |
Corrected Energy-72.1178 eV
Uncorrected energy = -72.8278 eV
Composition-based energy adjustment (0.071 eV/atom x 10.0 atoms) = 0.7100 eV
Corrected energy = -72.1178 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)