Final Magnetic Moment0.016 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-2.141 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.004 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. |
Density3.87 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMoO3 + K2Mo3O10 |
Band Gap2.941 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 MauguinPbca [61] |
Hall-P 2ac 2ab |
Point Groupmmm |
Crystal Systemorthorhombic |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 121.3 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 121.3 |
BN (mp-984) | <1 0 1> | <0 0 1> | 121.3 |
SiC (mp-7631) | <1 0 0> | <0 0 1> | 242.6 |
SiC (mp-7631) | <1 0 1> | <0 0 1> | 242.6 |
SiC (mp-7631) | <1 1 0> | <0 0 1> | 242.6 |
GaP (mp-2490) | <1 0 0> | <0 0 1> | 121.3 |
TbScO3 (mp-31119) | <1 1 0> | <0 1 1> | 190.2 |
NdGaO3 (mp-3196) | <1 1 0> | <0 0 1> | 121.3 |
Si (mp-149) | <1 0 0> | <0 0 1> | 121.3 |
SiC (mp-8062) | <1 1 0> | <0 0 1> | 242.6 |
TiO2 (mp-390) | <1 0 0> | <0 1 0> | 146.5 |
CsI (mp-614603) | <1 0 0> | <0 0 1> | 121.3 |
SrTiO3 (mp-4651) | <0 0 1> | <0 0 1> | 121.3 |
SrTiO3 (mp-4651) | <1 1 0> | <0 0 1> | 121.3 |
LiAlO2 (mp-3427) | <0 0 1> | <0 0 1> | 242.6 |
CaF2 (mp-2741) | <1 0 0> | <0 0 1> | 121.3 |
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 |
---|---|---|---|
Tl2Mo4O13 (mp-648007) | 0.2089 | 0.000 | 3 |
CsNbO3 (mp-27556) | 0.6485 | 0.000 | 3 |
K2Mo4O13 (mp-561805) | 0.5888 | 0.010 | 3 |
Tl2Mo7O22 (mp-704535) | 0.5541 | 0.015 | 3 |
Hg2W2O7 (mp-771222) | 0.6413 | 0.041 | 3 |
TlVTeO5 (mp-639714) | 0.6486 | 0.000 | 4 |
KSb(MoO4)2 (mp-618807) | 0.7165 | 0.020 | 4 |
RbMoIO6 (mp-568192) | 0.5990 | 0.000 | 4 |
Ba2YCu2F11 (mvc-9365) | 0.7116 | 0.055 | 4 |
LiV3(OF2)4 (mp-764216) | 0.7185 | 0.076 | 4 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesMo: 4.38 eV |
PseudopotentialsVASP PAW: K_sv Mo_pv O |
Final Energy/Atom-6.7030 eV |
Corrected Energy-1204.8797 eV
-1204.8797 eV = -1018.8495 eV (uncorrected energy) - 112.9920 eV (MP Advanced Correction) - 73.0382 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)