Final Magnetic Moment1.829 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFiM |
Formation Energy / Atom-2.076 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.066 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. |
Density8.31 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToW8O21 + WOF3 + W |
Band Gap0.000 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 MauguinPmma [51] |
Hall-P 2a 2a |
Point Groupmmm |
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] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <0 0 1> | 174.0 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 124.3 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 74.6 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 248.6 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 223.7 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 149.1 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 298.3 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 273.4 |
BaF2 (mp-1029) | <1 0 0> | <1 0 1> | 119.2 |
BaF2 (mp-1029) | <1 1 0> | <1 0 0> | 116.6 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 273.4 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 348.0 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 174.0 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 174.0 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 74.6 |
SiO2 (mp-6930) | <1 0 0> | <1 1 1> | 138.4 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 273.4 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 124.3 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 116.6 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 273.4 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 273.4 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 223.7 |
ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 273.4 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 273.4 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 223.7 |
CdS (mp-672) | <1 0 1> | <0 1 1> | 298.7 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 323.1 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 273.4 |
Te2W (mp-22693) | <1 0 0> | <0 0 1> | 99.4 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 124.3 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 298.3 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 198.8 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 323.1 |
Te2W (mp-22693) | <1 0 1> | <0 0 1> | 99.4 |
YVO4 (mp-19133) | <1 0 0> | <1 0 0> | 233.1 |
YVO4 (mp-19133) | <1 1 0> | <0 0 1> | 198.8 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 273.4 |
Te2Mo (mp-602) | <1 0 0> | <0 1 0> | 281.6 |
Te2Mo (mp-602) | <1 1 0> | <0 1 0> | 281.6 |
Te2Mo (mp-602) | <1 1 1> | <0 1 0> | 281.6 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 1 0> | 136.2 |
TePb (mp-19717) | <1 1 0> | <1 0 0> | 116.6 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 273.4 |
GaSe (mp-1943) | <1 0 0> | <0 1 0> | 70.4 |
GaSe (mp-1943) | <1 0 1> | <1 1 1> | 138.4 |
BN (mp-984) | <1 0 1> | <0 0 1> | 223.7 |
BN (mp-984) | <1 1 0> | <0 0 1> | 99.4 |
GaSe (mp-1943) | <0 0 1> | <0 1 1> | 74.7 |
BN (mp-984) | <0 0 1> | <0 0 1> | 273.4 |
BN (mp-984) | <1 0 0> | <0 0 1> | 99.4 |
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 |
---|---|---|---|
Sb3O7F (mp-753495) | 0.4620 | 0.040 | 3 |
Nb3O7F (mp-753459) | 0.4842 | 0.028 | 3 |
Nb5O12F (mp-759636) | 0.4633 | 0.043 | 3 |
Ta3O7F (mp-753747) | 0.4842 | 0.000 | 3 |
W3O7F (mp-765184) | 0.4412 | 0.026 | 3 |
U3O8 (mp-698) | 0.4675 | 0.003 | 2 |
U2O5 (mp-647814) | 0.4779 | 0.017 | 2 |
W3O8 (mp-715557) | 0.4779 | 0.004 | 2 |
U3O8 (mp-559906) | 0.4091 | 0.003 | 2 |
U3O8 (mp-560402) | 0.4807 | 0.012 | 2 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesW: 6.2 eV |
PseudopotentialsVASP PAW: W_pv O F |
Final Energy/Atom-7.3760 eV |
Corrected Energy-325.9002 eV
-325.9002 eV = -265.5352 eV (uncorrected energy) - 43.5100 eV (MP Advanced Correction) - 16.8550 eV (MP Anion 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)