Final Magnetic Moment1.002 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-2.391 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.027 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. |
Density2.86 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMo2P3O13 |
Band Gap0.099 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/c [15] |
Hall-C 2yc |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
CeO2 (mp-20194) | <1 0 0> | <0 1 1> | 177.4 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 316.5 |
GaN (mp-804) | <1 0 0> | <0 1 0> | 316.5 |
DyScO3 (mp-31120) | <0 1 0> | <0 1 1> | 177.4 |
CdS (mp-672) | <1 0 0> | <0 1 0> | 316.5 |
LiNbO3 (mp-3731) | <1 1 0> | <1 0 0> | 129.8 |
LiGaO2 (mp-5854) | <0 1 1> | <0 1 0> | 316.5 |
LiGaO2 (mp-5854) | <1 0 1> | <0 1 1> | 177.4 |
BaTiO3 (mp-5986) | <1 0 1> | <1 0 0> | 259.5 |
Si (mp-149) | <1 0 0> | <0 1 1> | 177.4 |
WS2 (mp-224) | <1 0 1> | <0 1 0> | 316.5 |
TiO2 (mp-2657) | <1 1 1> | <0 1 0> | 237.3 |
Mg (mp-153) | <1 0 1> | <0 1 0> | 316.5 |
KP(HO2)2 (mp-23959) | <0 1 0> | <0 0 1> | 158.8 |
MgF2 (mp-1249) | <0 0 1> | <1 0 -1> | 132.8 |
MgF2 (mp-1249) | <1 0 1> | <0 0 1> | 158.8 |
MgF2 (mp-1249) | <1 1 0> | <1 0 -1> | 265.6 |
Ni (mp-23) | <1 1 0> | <1 0 0> | 259.5 |
MoSe2 (mp-1634) | <0 0 1> | <0 1 0> | 316.5 |
WS2 (mp-224) | <1 1 0> | <0 0 1> | 158.8 |
WSe2 (mp-1821) | <0 0 1> | <0 1 0> | 316.5 |
YAlO3 (mp-3792) | <1 0 0> | <0 0 1> | 158.8 |
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 |
---|---|---|---|
P3W2O13 (mp-767436) | 0.4118 | 0.010 | 3 |
Mo2P3O13 (mp-504212) | 0.3830 | 0.054 | 3 |
Cr2P3O13 (mp-540528) | 0.2907 | 0.092 | 3 |
Mo2P3O13 (mp-540536) | 0.1957 | 0.009 | 3 |
Cr(PO4)2 (mp-697815) | 0.3751 | 0.189 | 3 |
LiMo2P3O13 (mp-705380) | 0.4660 | 0.054 | 4 |
LiP3W2O13 (mp-763650) | 0.4606 | 0.101 | 4 |
KMo2P3O13 (mp-566874) | 0.4493 | 0.000 | 4 |
NaMo2P3O13 (mp-566386) | 0.4641 | 0.000 | 4 |
CsNb(PO4)2 (mp-540750) | 0.4322 | 0.015 | 4 |
CsKMo4(P3O13)2 (mp-699557) | 0.4871 | 0.002 | 5 |
CsVGa(PO5)2 (mp-863295) | 0.5582 | 0.103 | 5 |
RbVGa(PO5)2 (mp-863294) | 0.6231 | 0.133 | 5 |
LiV2S2(O4F3)2 (mp-769600) | 0.6364 | 0.050 | 5 |
Na2Al2S3(Cl4O3)2 (mp-648140) | 0.6760 | 0.017 | 5 |
CsFeBP2HO9 (mp-761395) | 0.6748 | 0.119 | 6 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesMo: 4.38 eV |
PseudopotentialsVASP PAW: Mo_pv P O |
Final Energy/Atom-7.1725 eV |
Corrected Energy-290.5938 eV
-290.5938 eV = -258.2102 eV (uncorrected energy) - 18.2595 eV (MP Anion Correction) - 14.1240 eV (MP Advanced 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)