Final Magnetic Moment6.667 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-0.993 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.038 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. |
Density4.37 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMnS + Cr2S3 |
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 MauguinC2/m [12] |
Hall-C 2y |
Point Group2/m |
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 |
---|---|---|---|
Ti2VSe4 (mp-1025203) | 0.2812 | 0.016 | 3 |
Cr(MoS2)2 (mp-542188) | 0.2928 | 0.191 | 3 |
V2NiS4 (mp-4909) | 0.2882 | 0.002 | 3 |
V2CrS4 (mp-1078077) | 0.2642 | 0.087 | 3 |
V2FeS4 (mp-561419) | 0.2931 | 0.048 | 3 |
Li6Mn2O5F2 (mp-767468) | 0.6959 | 0.079 | 4 |
Li4Ti2Mn3O10 (mp-766150) | 0.6058 | 0.042 | 4 |
Li3TiMn3O8 (mp-765898) | 0.5797 | 0.066 | 4 |
Li6Fe(O2F)2 (mp-777322) | 0.6788 | 0.093 | 4 |
Li4Fe2Cu3O10 (mp-849416) | 0.6287 | 0.097 | 4 |
V3Se4 (mp-990764) | 0.3858 | 0.000 | 2 |
V3S4 (mp-850014) | 0.2669 | 0.020 | 2 |
Ti3Se4 (mp-1077978) | 0.3186 | 0.052 | 2 |
Fe3Se4 (mp-2780) | 0.3710 | 0.079 | 2 |
V3S4 (mp-1081) | 0.2972 | 0.020 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mn_pv Cr_pv S |
Final Energy/Atom-7.0441 eV |
Corrected Energy-51.9624 eV
-51.9624 eV = -49.3086 eV (uncorrected energy) - 2.6538 eV (MP Anion Correction)
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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)