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 / Atom0.096 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.210 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. |
Density2.41 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 MauguinCm [8] |
HallC 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 |
---|---|---|---|
Y5Mg8Cu5 (mp-646125) | 0.6368 | 0.001 | 3 |
CeZnRh (mp-607738) | 0.6460 | 0.000 | 3 |
Bi9Rh2Br3 (mp-680173) | 0.6349 | 0.029 | 3 |
LaMgRh (mp-569186) | 0.6281 | 0.000 | 3 |
LiYb2InGe2 (mp-977355) | 0.7067 | 0.000 | 4 |
Tb3Mn3Ga2Si (mp-22582) | 0.7398 | 0.346 | 4 |
Tm3Mn3Ga2Si (mp-570450) | 0.7370 | 0.090 | 4 |
LiCa2InGe2 (mp-570850) | 0.7193 | 0.000 | 4 |
Dy3Mn3Ga2Si (mp-21038) | 0.7396 | 0.322 | 4 |
Ga9Ir2 (mp-31311) | 0.5543 | 0.000 | 2 |
Ga9Rh2 (mp-31312) | 0.5367 | 0.000 | 2 |
Te4Pd9 (mp-29907) | 0.5478 | 0.000 | 2 |
MgSi (mp-1073722) | 0.6293 | 0.158 | 2 |
Mg4Si3 (mp-1074338) | 0.5942 | 0.164 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Si |
Final Energy/Atom-3.4168 eV |
Corrected Energy-41.0018 eV
-41.0018 eV = -41.0018 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)