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 / Atom0.118 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.218 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 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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
LiCuS (mp-766467) | 0.5936 | 0.040 | 3 |
Y2AlGe3 (mp-28997) | 0.5996 | 0.004 | 3 |
Ca3InAu3 (mp-606503) | 0.5413 | 0.000 | 3 |
Sm2AlGe3 (mp-568449) | 0.5958 | 0.004 | 3 |
Tb2AlGe3 (mp-571381) | 0.5950 | 0.005 | 3 |
K2BaCdSb2 (mp-863761) | 0.6698 | 0.000 | 4 |
K2SrCdSb2 (mp-863758) | 0.6324 | 0.000 | 4 |
KSr2Cd2Sb3 (mp-866639) | 0.7479 | 0.000 | 4 |
Mg3Si4 (mp-1075018) | 0.3839 | 0.222 | 2 |
Mg3Si4 (mp-1075277) | 0.5189 | 0.188 | 2 |
Mg3Si4 (mp-1075269) | 0.5505 | 0.202 | 2 |
Mg5Si6 (mp-1075481) | 0.4778 | 0.157 | 2 |
Mg6Si5 (mp-1073934) | 0.5322 | 0.199 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Si |
Final Energy/Atom-3.6655 eV |
Corrected Energy-50.7487 eV
Uncorrected energy = -51.3167 eV
Composition-based energy adjustment (0.071 eV/atom x 8.0 atoms) = 0.5680 eV
Corrected energy = -50.7487 eV
|
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)