Final Magnetic Moment0.999 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-1.196 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 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. |
Density4.77 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
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 MauguinR3 [148] |
Hall-R 3 |
Point Group3 |
Crystal Systemtrigonal |
Topological ClassificationSM*
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SubclassificationESFD†
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Crossing TypePoint
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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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
CeO2 (mp-20194) | <1 1 0> | <1 0 0> | 169.6 |
BaF2 (mp-1029) | <1 1 0> | <1 0 0> | 169.6 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 169.6 |
SiC (mp-7631) | <1 1 0> | <1 0 0> | 169.6 |
GaP (mp-2490) | <1 1 0> | <1 0 0> | 169.6 |
NdGaO3 (mp-3196) | <0 1 0> | <1 0 0> | 169.6 |
Si (mp-149) | <1 1 0> | <1 0 0> | 169.6 |
YAlO3 (mp-3792) | <0 0 1> | <1 0 0> | 169.6 |
AlN (mp-661) | <0 0 1> | <1 0 0> | 169.6 |
ZrO2 (mp-2858) | <1 0 0> | <1 0 0> | 169.6 |
CsI (mp-614603) | <1 1 0> | <1 0 0> | 169.6 |
CaF2 (mp-2741) | <1 1 0> | <1 0 0> | 169.6 |
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 |
---|---|---|---|
Pr7FeI12 (mp-638650) | 0.2463 | 0.001 | 3 |
Pr7CoI12 (mp-569261) | 0.1459 | 0.000 | 3 |
Ho7FeI12 (mp-567566) | 0.0956 | 0.000 | 3 |
Sc7CoI12 (mp-541175) | 0.2849 | 0.000 | 3 |
Sc7NCl12 (mp-29579) | 0.2949 | 0.001 | 3 |
Li2NbOF5 (mp-755505) | 0.5112 | 0.008 | 4 |
SrLa6OsI12 (mp-567419) | 0.2435 | 0.000 | 4 |
Li2NbOF5 (mp-756639) | 0.5192 | 0.010 | 4 |
NaLa6OsI12 (mp-569905) | 0.3133 | 0.000 | 4 |
UHg3(TeCl3)2 (mp-567543) | 0.5350 | 0.000 | 4 |
Tl2S (mp-667) | 0.5751 | 0.001 | 2 |
In7Cl9 (mp-28730) | 0.5514 | 0.000 | 2 |
Pd2N (mp-510087) | 0.5916 | 0.514 | 2 |
Tl2S (mp-556516) | 0.5751 | 0.000 | 2 |
In7Br9 (mp-28988) | 0.5654 | 0.010 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Y_sv Fe_pv I |
Final Energy/Atom-4.7976 eV |
Corrected Energy-95.9515 eV
-95.9515 eV = -95.9515 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)