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-2.921 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.003 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. |
Density7.50 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToWO3 + Ta2O5 |
Band Gap1.798 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 MauguinPc [7] |
HallP 2yc |
Point Groupm |
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] |
---|---|---|---|
AlN (mp-661) | <1 0 1> | <0 1 0> | 263.3 |
CeO2 (mp-20194) | <1 0 0> | <0 1 0> | 263.3 |
CeO2 (mp-20194) | <1 1 1> | <0 1 0> | 263.3 |
GaN (mp-804) | <1 1 0> | <0 1 0> | 263.3 |
KTaO3 (mp-3614) | <1 1 1> | <0 1 0> | 329.1 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 131.7 |
DyScO3 (mp-31120) | <1 0 1> | <0 1 0> | 329.1 |
Te2W (mp-22693) | <0 1 0> | <0 1 0> | 263.3 |
Te2Mo (mp-602) | <1 1 0> | <0 0 1> | 281.5 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 1 0> | 263.3 |
GaSe (mp-1943) | <1 0 1> | <0 1 1> | 289.1 |
Te2Mo (mp-602) | <1 0 0> | <0 1 0> | 263.3 |
Ag (mp-124) | <1 1 0> | <0 1 0> | 197.5 |
GaSe (mp-1943) | <0 0 1> | <0 1 0> | 329.1 |
GaSe (mp-1943) | <1 0 0> | <0 0 1> | 70.4 |
BN (mp-984) | <0 0 1> | <0 1 1> | 289.1 |
Al (mp-134) | <1 1 1> | <0 1 0> | 329.1 |
TeO2 (mp-2125) | <1 0 0> | <0 1 1> | 289.1 |
MgO (mp-1265) | <1 0 0> | <0 1 0> | 329.1 |
TiO2 (mp-2657) | <1 0 1> | <0 1 0> | 329.1 |
C (mp-66) | <1 1 0> | <0 1 0> | 197.5 |
GdScO3 (mp-5690) | <1 0 1> | <0 1 0> | 329.1 |
Mg (mp-153) | <1 1 0> | <0 1 0> | 263.3 |
GdScO3 (mp-5690) | <0 1 1> | <0 1 0> | 329.1 |
GdScO3 (mp-5690) | <1 1 0> | <0 1 1> | 192.7 |
Mg (mp-153) | <1 0 1> | <0 0 1> | 281.5 |
GaP (mp-2490) | <1 1 0> | <0 1 0> | 131.7 |
GaP (mp-2490) | <1 1 1> | <0 1 0> | 263.3 |
InP (mp-20351) | <1 1 0> | <0 1 0> | 197.5 |
TbScO3 (mp-31119) | <1 0 0> | <0 1 0> | 131.7 |
TbScO3 (mp-31119) | <1 0 1> | <0 1 0> | 329.1 |
Ni (mp-23) | <1 1 0> | <0 1 0> | 263.3 |
BaTiO3 (mp-5986) | <1 1 1> | <0 1 0> | 263.3 |
NdGaO3 (mp-3196) | <1 0 0> | <0 1 0> | 131.7 |
NdGaO3 (mp-3196) | <1 0 1> | <0 1 0> | 329.1 |
Ga2O3 (mp-886) | <1 0 0> | <0 1 1> | 289.1 |
Ga2O3 (mp-886) | <1 1 0> | <0 1 1> | 289.1 |
MoSe2 (mp-1634) | <1 0 0> | <0 1 0> | 263.3 |
MoSe2 (mp-1634) | <1 1 0> | <0 1 0> | 263.3 |
Si (mp-149) | <1 0 0> | <0 1 0> | 263.3 |
Au (mp-81) | <1 1 0> | <0 1 0> | 197.5 |
Ga2O3 (mp-886) | <0 1 0> | <0 1 1> | 289.1 |
Si (mp-149) | <1 1 1> | <0 1 0> | 263.3 |
ZrO2 (mp-2858) | <1 1 -1> | <0 1 0> | 329.1 |
ZrO2 (mp-2858) | <1 1 1> | <0 1 0> | 263.3 |
C (mp-48) | <1 0 0> | <0 1 0> | 131.7 |
ZrO2 (mp-2858) | <0 1 1> | <0 0 1> | 281.5 |
CaCO3 (mp-3953) | <1 0 0> | <0 1 0> | 263.3 |
CaCO3 (mp-3953) | <1 0 1> | <0 0 1> | 281.5 |
SiC (mp-8062) | <1 1 0> | <0 1 0> | 329.1 |
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 |
---|---|---|---|
SrLaCl5 (mp-768597) | 0.6784 | 0.073 | 3 |
Na3(W3O8)4 (mp-780475) | 0.6462 | 0.031 | 3 |
BaTa6O16 (mp-769349) | 0.5741 | 0.000 | 3 |
K2Mo7O20 (mp-579220) | 0.6078 | 0.006 | 3 |
Nb6CdO16 (mp-773090) | 0.5319 | 0.049 | 3 |
U2O5 (mp-647814) | 0.5969 | 0.017 | 2 |
W18O49 (mp-19529) | 0.3337 | 0.000 | 2 |
W8O21 (mp-579377) | 0.3486 | 0.000 | 2 |
W18O49 (mp-567091) | 0.3335 | 0.000 | 2 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesW: 6.2 eV |
PseudopotentialsVASP PAW: Ta_pv W_pv O |
Final Energy/Atom-8.9470 eV |
Corrected Energy-867.0916 eV
-867.0916 eV = -787.3371 eV (uncorrected energy) - 44.9466 eV (MP Anion Correction) - 34.8080 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)