Final Magnetic Moment1.003 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-0.639 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.827 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. |
Density2.81 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMn8Cl3O10 + Cl2O + MnCl2 |
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 |
---|---|---|---|
Rb3Au3Cl8 (mp-27301) | 0.6458 | 0.000 | 3 |
FeHO2 (mp-542980) | 0.6373 | 0.051 | 3 |
Mg(BrO)2 (mp-1069922) | 0.5431 | 1.246 | 3 |
Fe(BrN)2 (mp-1079633) | 0.5418 | 1.211 | 3 |
AlHO2 (mp-23807) | 0.6325 | 0.034 | 3 |
Cu2H3ClO3 (mp-642737) | 0.7163 | 0.051 | 4 |
KTeOF3 (mp-612946) | 0.7408 | 0.107 | 4 |
Tl2Pt(CN)4 (mp-621092) | 0.6637 | 0.061 | 4 |
KI(OF)2 (mp-558861) | 0.7449 | 0.000 | 4 |
MgSi(HO2)2 (mp-1078877) | 0.7442 | 0.152 | 4 |
Te3Cl2 (mp-27628) | 0.7246 | 0.013 | 2 |
SeF4 (mp-29172) | 0.7096 | 0.000 | 2 |
Na2MoC3SeN3 (mp-683943) | 0.6302 | 0.071 | 5 |
Rb2PtC4(BrN2)2 (mp-571526) | 0.7167 | 0.219 | 5 |
K2PtC4(BrN2)2 (mp-568299) | 0.6979 | 0.225 | 5 |
K2PtC4(IN2)2 (mp-570105) | 0.6087 | 0.204 | 5 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesMn: 3.9 eV |
PseudopotentialsVASP PAW: Mn_pv Cl O |
Final Energy/Atom-4.0728 eV |
Corrected Energy-23.4494 eV
-23.4494 eV = -20.3640 eV (uncorrected energy) - 1.6809 eV (MP Advanced Correction) - 1.4046 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)