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 OrderingNM |
Formation Energy / Atom-2.538 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.045 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. |
Density2.49 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToVP2O7 + LiPO3 + VPO5 + O2 |
Band Gap0.588 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 MauguinP1 [1] |
HallP 1 |
Point Group1 |
Crystal Systemtriclinic |
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] |
---|---|---|---|
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 140.4 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 139.6 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 164.4 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 139.6 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 164.4 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 82.2 |
YVO4 (mp-19133) | <1 0 1> | <0 1 0> | 139.6 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 139.6 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 0> | 139.6 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 246.7 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 246.7 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 139.6 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 246.7 |
GdScO3 (mp-5690) | <1 0 0> | <0 1 0> | 139.6 |
GdScO3 (mp-5690) | <1 0 1> | <0 0 1> | 164.4 |
Al (mp-134) | <1 1 0> | <0 1 0> | 139.6 |
Ni (mp-23) | <1 0 0> | <0 0 1> | 246.7 |
GdScO3 (mp-5690) | <0 1 1> | <0 0 1> | 164.4 |
Mg (mp-153) | <0 0 1> | <0 0 1> | 246.7 |
PbS (mp-21276) | <1 1 1> | <0 0 1> | 246.7 |
InP (mp-20351) | <1 1 1> | <0 0 1> | 246.7 |
TbScO3 (mp-31119) | <0 1 1> | <0 0 1> | 164.4 |
TbScO3 (mp-31119) | <1 0 0> | <0 1 0> | 139.6 |
TbScO3 (mp-31119) | <1 0 1> | <0 0 1> | 164.4 |
NaCl (mp-22862) | <1 1 0> | <0 1 0> | 139.6 |
ZrO2 (mp-2858) | <1 1 0> | <0 1 1> | 162.0 |
Ni (mp-23) | <1 1 0> | <0 1 0> | 139.6 |
BaTiO3 (mp-5986) | <1 0 1> | <0 1 0> | 139.6 |
NdGaO3 (mp-3196) | <0 1 1> | <0 0 1> | 164.4 |
NdGaO3 (mp-3196) | <1 0 1> | <0 0 1> | 164.4 |
WS2 (mp-224) | <0 0 1> | <0 0 1> | 246.7 |
WS2 (mp-224) | <1 0 0> | <0 1 0> | 139.6 |
SrTiO3 (mp-4651) | <1 0 1> | <0 0 1> | 164.4 |
Ge (mp-32) | <1 1 0> | <0 1 0> | 139.6 |
Al2O3 (mp-1143) | <0 0 1> | <1 0 1> | 161.6 |
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 |
---|---|---|---|
SnP2O7 (mvc-5322) | 0.5053 | 0.111 | 3 |
Mn7Cr12O48 (mp-774029) | 0.5016 | 0.078 | 3 |
V(PO3)3 (mp-705305) | 0.5019 | 0.072 | 3 |
Cr(PO3)3 (mp-31690) | 0.4883 | 0.093 | 3 |
Cr(PO3)3 (mp-694576) | 0.4897 | 0.093 | 3 |
Li3V3P8O29 (mp-865197) | 0.1277 | 0.041 | 4 |
Li3V3P8O29 (mp-764123) | 0.1475 | 0.045 | 4 |
Li3V3P8O29 (mp-764122) | 0.0919 | 0.046 | 4 |
Li3V3P8O29 (mp-865196) | 0.1426 | 0.044 | 4 |
Li3V3P8O29 (mp-761942) | 0.1591 | 0.042 | 4 |
Cr19O48 (mp-850874) | 0.5091 | 0.097 | 2 |
V5O12 (mp-776915) | 0.7080 | 0.032 | 2 |
Cr19O48 (mp-780521) | 0.5163 | 0.085 | 2 |
Cr5O12 (mp-19575) | 0.7293 | 0.025 | 2 |
LiBS4(ClO3)4 (mp-555090) | 0.6130 | 0.005 | 5 |
LiSn2P4H3O16 (mp-754500) | 0.5767 | 0.059 | 5 |
LiVSO4F3 (mp-769603) | 0.6152 | 0.048 | 5 |
SnP4H8N2O13 (mp-603633) | 0.4335 | 0.010 | 5 |
TiP4H8N2O13 (mp-603612) | 0.5519 | 0.026 | 5 |
VBP2H5NO9 (mp-25798) | 0.6276 | 0.000 | 6 |
RbScBP2HO9 (mp-23809) | 0.6311 | 0.000 | 6 |
CsAlBP2HO9 (mp-542129) | 0.6268 | 0.000 | 6 |
RbAlBP2HO9 (mp-542130) | 0.5948 | 0.000 | 6 |
NaMgAl3Si8(HO6)4 (mp-1094103) | 0.5135 | 0.027 | 6 |
Al2P2H8C2NO8F (mp-708964) | 0.5896 | 0.050 | 7 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesV: 3.25 eV |
PseudopotentialsVASP PAW: Li_sv V_pv P O |
Final Energy/Atom-7.0584 eV |
Corrected Energy-657.8438 eV
-657.8438 eV = -607.0190 eV (uncorrected energy) - 40.7328 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)