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 OrderingAFM |
Formation Energy / Atom-1.960 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.008 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. |
Density4.59 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMo8O23 + TeO2 + MoO2 |
Band Gap1.374 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 MauguinP21/c [14] |
Hall-P 2ybc |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <1 0 1> | <0 1 0> | 252.9 |
SiO2 (mp-6930) | <0 0 1> | <1 1 0> | 174.2 |
DyScO3 (mp-31120) | <1 1 0> | <0 1 0> | 252.9 |
CdS (mp-672) | <1 0 1> | <0 1 0> | 252.9 |
LiF (mp-1138) | <1 1 1> | <1 1 0> | 174.2 |
Ag (mp-124) | <1 1 0> | <0 1 1> | 148.0 |
AlN (mp-661) | <1 0 0> | <0 1 0> | 252.9 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 243.3 |
BN (mp-984) | <1 1 1> | <0 0 1> | 243.3 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 174.2 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 121.7 |
Bi2Se3 (mp-541837) | <1 0 0> | <0 1 0> | 252.9 |
LiGaO2 (mp-5854) | <0 1 1> | <1 1 0> | 174.2 |
LiGaO2 (mp-5854) | <1 1 0> | <1 0 1> | 196.3 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 121.7 |
Te2W (mp-22693) | <0 1 1> | <0 1 0> | 168.6 |
SiC (mp-7631) | <1 1 0> | <0 0 1> | 243.3 |
MgO (mp-1265) | <1 1 0> | <1 0 0> | 152.5 |
MgO (mp-1265) | <1 1 1> | <0 1 0> | 252.9 |
TiO2 (mp-2657) | <1 1 0> | <1 0 1> | 196.3 |
C (mp-66) | <1 0 0> | <1 0 0> | 152.5 |
C (mp-66) | <1 1 0> | <0 1 0> | 252.9 |
Mg (mp-153) | <1 1 0> | <1 1 0> | 174.2 |
GdScO3 (mp-5690) | <1 1 1> | <0 1 1> | 148.0 |
InP (mp-20351) | <1 1 0> | <0 1 1> | 148.0 |
PbS (mp-21276) | <1 1 0> | <1 0 0> | 152.5 |
BaTiO3 (mp-5986) | <1 1 1> | <1 1 0> | 174.2 |
InP (mp-20351) | <1 1 1> | <0 0 1> | 121.7 |
Au (mp-81) | <1 1 0> | <0 1 1> | 148.0 |
SiC (mp-11714) | <1 0 0> | <0 1 0> | 252.9 |
SiC (mp-11714) | <1 1 0> | <0 1 0> | 168.6 |
WSe2 (mp-1821) | <1 0 0> | <1 0 0> | 152.5 |
Ge(Bi3O5)4 (mp-23352) | <1 1 0> | <1 0 0> | 152.5 |
CaCO3 (mp-3953) | <1 0 0> | <1 1 0> | 174.2 |
ZrO2 (mp-2858) | <1 0 1> | <0 1 0> | 84.3 |
YAlO3 (mp-3792) | <0 1 0> | <1 0 0> | 152.5 |
CdWO4 (mp-19387) | <0 0 1> | <0 1 0> | 252.9 |
CdWO4 (mp-19387) | <1 0 0> | <0 1 0> | 252.9 |
GaTe (mp-542812) | <1 0 -1> | <0 1 1> | 148.0 |
TiO2 (mp-390) | <1 1 1> | <0 1 0> | 168.6 |
LiAlO2 (mp-3427) | <1 0 0> | <0 1 0> | 168.6 |
Al2O3 (mp-1143) | <0 0 1> | <0 0 1> | 121.7 |
GaTe (mp-542812) | <0 0 1> | <0 1 1> | 148.0 |
LiAlO2 (mp-3427) | <1 0 1> | <0 1 0> | 84.3 |
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 |
---|---|---|---|
Sb2Mo10O31 (mp-609510) | 0.4078 | 0.011 | 3 |
Hg2W2O7 (mp-773392) | 0.3621 | 0.008 | 3 |
Hg2W2O7 (mp-774407) | 0.3838 | 0.007 | 3 |
Hg2Mo2O7 (mp-32131) | 0.5033 | 0.004 | 3 |
Hg2Mo2O7 (mp-566945) | 0.4906 | 0.003 | 3 |
LiV(OF)2 (mp-765956) | 0.6360 | 0.000 | 4 |
LiV4O5F7 (mp-777081) | 0.6975 | 0.084 | 4 |
K2Te(WO4)3 (mp-566368) | 0.6143 | 0.001 | 4 |
Ag2Mo3SeO12 (mp-566624) | 0.6755 | 0.009 | 4 |
RbV2I3O13 (mp-566106) | 0.6029 | 0.000 | 4 |
Mo9O26 (mp-706490) | 0.7310 | 0.043 | 2 |
MoO3 (mp-715463) | 0.7142 | 0.038 | 2 |
V5O12 (mp-777580) | 0.7222 | 0.071 | 2 |
MoO3 (mp-510584) | 0.7193 | 0.039 | 2 |
V2O5 (mp-542844) | 0.7037 | 0.061 | 2 |
K2FeH2Cl5O (mp-25745) | 0.7487 | 0.000 | 5 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesMo: 4.38 eV |
PseudopotentialsVASP PAW: Te Mo_pv O |
Final Energy/Atom-6.8528 eV |
Corrected Energy-711.0582 eV
Uncorrected energy = -603.0502 eV
Composition-based energy adjustment (-0.687 eV/atom x 64.0 atoms) = -43.9680 eV
Composition-based energy adjustment (-3.202 eV/atom x 20.0 atoms) = -64.0400 eV
Corrected energy = -711.0582 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)