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 / Atom-1.881 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.224 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. |
Density3.36 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToFeO + CaS |
Band Gap1.151 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 MauguinP63mc [186] |
HallP 6c 2c |
Point Group6mm |
Crystal Systemhexagonal |
Topological Classificationtrivial*
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SubclassificationLCEBR†
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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 |
---|---|---|---|
Tl2CdTe4 (mp-1025337) | 0.4114 | 0.098 | 3 |
Sn(HgSe2)2 (mp-10955) | 0.3960 | 0.000 | 3 |
Mg(InTe2)2 (mp-35777) | 0.4216 | 0.005 | 3 |
LiMnSe2 (mp-10231) | 0.4266 | 0.094 | 3 |
Tl2CdTe4 (mp-1025299) | 0.3998 | 0.096 | 3 |
CaZnSO (mp-7204) | 0.1692 | 0.010 | 4 |
LiCoPO4 (mp-761965) | 0.6723 | 0.087 | 4 |
LiNiPO4 (mp-767987) | 0.6445 | 0.067 | 4 |
CdGe(BiO3)2 (mp-555027) | 0.6904 | 0.000 | 4 |
LiMnPO4 (mp-765826) | 0.7011 | 0.059 | 4 |
Ge3As4 (mp-569600) | 0.5107 | 0.041 | 2 |
Sn3As4 (mp-570377) | 0.5856 | 0.035 | 2 |
As4C3 (mp-568505) | 0.4589 | 0.874 | 2 |
Si3As4 (mp-570744) | 0.4734 | 0.059 | 2 |
GeP (mp-1095275) | 0.4875 | 0.015 | 2 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesFe: 5.3 eV |
PseudopotentialsVASP PAW: Ca_sv Fe_pv S O |
Final Energy/Atom-4.9382 eV |
Corrected Energy-46.3977 eV
Uncorrected energy = -39.5057 eV
Composition-based energy adjustment (-0.503 eV/atom x 2.0 atoms) = -1.0060 eV
Composition-based energy adjustment (-0.687 eV/atom x 2.0 atoms) = -1.3740 eV
Composition-based energy adjustment (-2.256 eV/atom x 2.0 atoms) = -4.5120 eV
Corrected energy = -46.3977 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)