Final Magnetic Moment5.002 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-2.629 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. |
Density2.47 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToVP2O7 + V(PO3)3 + VPO4 |
Band Gap0.004 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 MauguinAea2 [41] |
HallA 2 2ac |
Point Groupmm2 |
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] |
---|---|---|---|
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 140.3 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 140.3 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 140.3 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 257.8 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 140.3 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 175.5 |
YVO4 (mp-19133) | <1 1 0> | <0 0 1> | 128.9 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 257.8 |
Al (mp-134) | <1 1 0> | <0 1 0> | 140.3 |
LiGaO2 (mp-5854) | <0 1 0> | <0 0 1> | 128.9 |
Ni (mp-23) | <1 1 0> | <0 1 0> | 140.3 |
SiC (mp-11714) | <1 0 0> | <0 1 1> | 190.5 |
NaCl (mp-22862) | <1 1 0> | <0 1 0> | 140.3 |
LiTaO3 (mp-3666) | <1 0 0> | <0 1 0> | 140.3 |
MoSe2 (mp-1634) | <1 0 0> | <0 0 1> | 257.8 |
YAlO3 (mp-3792) | <0 1 1> | <0 1 1> | 190.5 |
MgF2 (mp-1249) | <1 0 0> | <1 0 0> | 175.5 |
Ge (mp-32) | <1 1 0> | <0 1 0> | 140.3 |
Fe2O3 (mp-24972) | <1 0 0> | <0 1 0> | 140.3 |
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 |
---|---|---|---|
TiP2O7 (mp-26630) | 0.2936 | 0.007 | 3 |
V3(P3O10)2 (mp-32504) | 0.2301 | 0.023 | 3 |
MgP4O11 (mp-15437) | 0.3081 | 0.000 | 3 |
Fe3(P3O10)2 (mp-31877) | 0.2206 | 0.169 | 3 |
Co3(P3O10)2 (mp-31597) | 0.2579 | 0.131 | 3 |
VFe(P2O7)2 (mp-767722) | 0.2756 | 0.009 | 4 |
VCr(P2O7)2 (mp-767779) | 0.3040 | 0.021 | 4 |
LiP4WO12 (mp-763455) | 0.2826 | 0.017 | 4 |
CsV2P5O16 (mp-541176) | 0.3141 | 0.001 | 4 |
LiNb(PO3)4 (mp-757816) | 0.2832 | 0.118 | 4 |
Cr5O12 (mp-773920) | 0.7465 | 0.000 | 2 |
Nb2O5 (mp-776896) | 0.6187 | 0.059 | 2 |
V5O12 (mp-778252) | 0.7376 | 0.024 | 2 |
MgCr3Se2(SO6)4 (mp-769544) | 0.5900 | 0.126 | 5 |
LiVP3HO10 (mp-763631) | 0.6086 | 0.080 | 5 |
MgCr3Se3(SO8)3 (mp-773999) | 0.5678 | 0.180 | 5 |
CsGaP3HO10 (mp-703308) | 0.5894 | 0.000 | 5 |
KMnP3HO10 (mp-542842) | 0.6232 | 0.000 | 5 |
CsAlBP2HO9 (mp-542129) | 0.7367 | 0.000 | 6 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesV: 3.25 eV |
PseudopotentialsVASP PAW: V_pv P O |
Final Energy/Atom-7.4425 eV |
Corrected Energy-469.8502 eV
-469.8502 eV = -431.6666 eV (uncorrected energy) - 28.0916 eV (MP Anion Correction) - 10.0920 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)