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 / Atom0.109 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.185 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. |
Density2.39 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 [2] |
Hall-P 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 |
---|---|---|---|
KCu3S2 (mp-9868) | 0.6098 | 0.004 | 3 |
Tl3AgTe2 (mp-650442) | 0.5929 | 0.000 | 3 |
CoAsS (mp-613314) | 0.6023 | 0.298 | 3 |
KSm2Cl5 (mp-568044) | 0.5941 | 0.091 | 3 |
K3In2As3 (mp-583615) | 0.5924 | 0.000 | 3 |
TiTlCuTe3 (mp-9344) | 0.6939 | 0.000 | 4 |
Rb2CeCu3Te5 (mp-581778) | 0.7015 | 0.093 | 4 |
Sm3NbSe3O4 (mp-555559) | 0.7276 | 0.024 | 4 |
Nb2Tl3CuSe12 (mp-570757) | 0.7199 | 0.000 | 4 |
KSr2Cd2Sb3 (mp-866639) | 0.6747 | 0.000 | 4 |
Mg2Si3 (mp-1073059) | 0.5145 | 0.178 | 2 |
Mg2Si3 (mp-1073199) | 0.5251 | 0.221 | 2 |
MgSi2 (mp-1073294) | 0.5419 | 0.186 | 2 |
Mg2Si3 (mp-1073438) | 0.5412 | 0.264 | 2 |
Mg3Si4 (mp-1074934) | 0.5174 | 0.199 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Si |
Final Energy/Atom-4.0411 eV |
Corrected Energy-48.4937 eV
-48.4937 eV = -48.4937 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)