Final Magnetic Moment0.500 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-1.924 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.030 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. |
Density9.60 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToW8O21 + 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 MauguinP42/mnm [136] |
Hall-P 4n 2n |
Point Groupmmm |
Crystal Systemtetragonal |
Topological ClassificationTI*
|
SubclassificationNLC†
|
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
Apply Gaussian smoothing:
Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | elastic energy [meV] | MCIA† [Å2] |
---|---|---|---|---|
Ge3(BiO3)4 (mp-23560) | <1 0 0> | <0 0 1> | 0.000 | 113.7 |
KP(HO2)2 (mp-23959) | <0 0 1> | <0 0 1> | 0.001 | 227.5 |
Te2W (mp-22693) | <0 0 1> | <1 1 1> | 0.008 | 222.2 |
GdScO3 (mp-5690) | <0 1 0> | <1 0 0> | 0.013 | 266.2 |
BN (mp-984) | <1 0 0> | <1 0 1> | 0.014 | 193.3 |
BN (mp-984) | <0 0 1> | <1 0 0> | 0.016 | 109.6 |
MgO (mp-1265) | <1 0 0> | <0 0 1> | 0.018 | 91.0 |
Ge (mp-32) | <1 0 0> | <1 0 1> | 0.027 | 165.7 |
GaAs (mp-2534) | <1 0 0> | <1 0 1> | 0.029 | 165.7 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 0> | 0.029 | 140.9 |
ZnSe (mp-1190) | <1 0 0> | <1 0 1> | 0.047 | 165.7 |
Al2O3 (mp-1143) | <1 0 0> | <1 0 0> | 0.050 | 62.6 |
Al2O3 (mp-1143) | <1 0 1> | <1 0 0> | 0.051 | 266.2 |
CdWO4 (mp-19387) | <0 0 1> | <1 1 0> | 0.058 | 243.6 |
NdGaO3 (mp-3196) | <0 1 1> | <1 0 0> | 0.064 | 156.6 |
KP(HO2)2 (mp-23959) | <1 0 0> | <0 0 1> | 0.071 | 113.7 |
WS2 (mp-224) | <1 1 1> | <1 1 1> | 0.072 | 158.7 |
KP(HO2)2 (mp-23959) | <0 1 0> | <0 0 1> | 0.076 | 227.5 |
GaTe (mp-542812) | <1 0 0> | <1 0 0> | 0.076 | 313.2 |
TbScO3 (mp-31119) | <1 1 1> | <1 0 0> | 0.078 | 140.9 |
GdScO3 (mp-5690) | <0 0 1> | <1 0 1> | 0.082 | 193.3 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 0.090 | 62.6 |
Mg (mp-153) | <0 0 1> | <1 1 1> | 0.109 | 158.7 |
C (mp-66) | <1 0 0> | <0 0 1> | 0.113 | 113.7 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 1> | 0.118 | 55.2 |
MoSe2 (mp-1634) | <0 0 1> | <1 1 1> | 0.121 | 95.2 |
WSe2 (mp-1821) | <0 0 1> | <1 1 1> | 0.122 | 95.2 |
LiGaO2 (mp-5854) | <1 1 1> | <1 1 0> | 0.124 | 110.7 |
Ga2O3 (mp-886) | <1 1 0> | <1 0 0> | 0.137 | 219.2 |
ZnO (mp-2133) | <1 0 1> | <1 0 0> | 0.146 | 78.3 |
CdS (mp-672) | <1 0 1> | <1 0 1> | 0.150 | 193.3 |
Au (mp-81) | <1 1 1> | <1 1 0> | 0.156 | 243.6 |
YAlO3 (mp-3792) | <0 1 0> | <1 0 1> | 0.157 | 276.2 |
CdWO4 (mp-19387) | <1 1 0> | <1 1 0> | 0.163 | 287.9 |
NdGaO3 (mp-3196) | <1 0 0> | <1 0 0> | 0.164 | 266.2 |
MoSe2 (mp-1634) | <1 0 1> | <1 0 0> | 0.181 | 156.6 |
Te2W (mp-22693) | <1 0 0> | <1 0 1> | 0.181 | 193.3 |
TbScO3 (mp-31119) | <1 0 1> | <1 0 1> | 0.194 | 55.2 |
ZrO2 (mp-2858) | <0 1 1> | <1 1 0> | 0.195 | 155.0 |
SiC (mp-7631) | <0 0 1> | <1 0 0> | 0.206 | 125.3 |
Fe3O4 (mp-19306) | <1 0 0> | <0 0 1> | 0.210 | 295.7 |
SiC (mp-11714) | <0 0 1> | <1 0 0> | 0.210 | 125.3 |
MoSe2 (mp-1634) | <1 1 1> | <1 0 0> | 0.211 | 266.2 |
TbScO3 (mp-31119) | <0 1 0> | <1 0 0> | 0.215 | 266.2 |
LiF (mp-1138) | <1 1 0> | <1 1 1> | 0.217 | 95.2 |
TiO2 (mp-390) | <1 0 0> | <1 0 1> | 0.221 | 110.5 |
Ga2O3 (mp-886) | <1 0 0> | <1 0 0> | 0.223 | 125.3 |
TeO2 (mp-2125) | <1 0 0> | <1 1 1> | 0.227 | 285.7 |
InSb (mp-20012) | <1 1 0> | <1 0 0> | 0.236 | 62.6 |
CdTe (mp-406) | <1 1 1> | <0 0 1> | 0.239 | 227.5 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
CrWO4 (mp-18785) | 0.0677 | 0.000 | 3 |
LiAg2F6 (mp-753881) | 0.0876 | 0.042 | 3 |
CrIrO4 (mp-769670) | 0.0995 | 0.000 | 3 |
MnCoO4 (mp-761556) | 0.1186 | 0.306 | 3 |
CrSbO4 (mp-774944) | 0.1055 | 0.000 | 3 |
LiFe3(OF3)2 (mp-779990) | 0.2754 | 0.005 | 4 |
LiV3(OF3)2 (mp-868491) | 0.2138 | 0.000 | 4 |
LiFe2OF5 (mp-779300) | 0.2758 | 0.244 | 4 |
LiCo3(OF3)2 (mp-850982) | 0.2395 | 0.022 | 4 |
Ta2CrNO5 (mp-849504) | 0.2426 | 0.065 | 4 |
FeF2 (mp-556911) | 0.1180 | 0.000 | 2 |
WO2 (mvc-6930) | 0.0360 | 0.030 | 2 |
MoO2 (mp-510536) | 0.0621 | 0.000 | 2 |
MoO2 (mp-566458) | 0.0795 | 0.000 | 2 |
VO2 (mp-19094) | 0.1305 | 0.000 | 2 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesW: 6.2 eV |
PseudopotentialsVASP PAW: W_pv O |
Final Energy/Atom-7.6236 eV |
Corrected Energy-114.5055 eV
-114.5055 eV = -91.4832 eV (uncorrected energy) - 17.4040 eV (MP Advanced Correction) - 5.6183 eV (MP Anion Correction)
|
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)