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-0.145 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 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. |
Density13.52 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
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 MauguinFd3m [227] |
HallF 4d 2 3 1d |
Point Groupm3m |
Crystal Systemcubic |
Topological ClassificationSM*
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SubclassificationESFD†
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Crossing TypePoint
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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.
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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] |
---|---|---|---|---|
Cu (mp-30) | <1 0 0> | <1 0 0> | 0.001 | 117.6 |
Cu (mp-30) | <1 1 0> | <1 1 0> | 0.001 | 166.3 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 0.001 | 294.0 |
AlN (mp-661) | <0 0 1> | <1 1 1> | 0.002 | 101.8 |
Al (mp-134) | <1 0 0> | <1 0 0> | 0.002 | 294.0 |
MgO (mp-1265) | <1 0 0> | <1 0 0> | 0.003 | 235.2 |
InSb (mp-20012) | <1 1 0> | <1 1 0> | 0.007 | 249.5 |
CdTe (mp-406) | <1 1 0> | <1 1 0> | 0.018 | 249.5 |
LaAlO3 (mp-2920) | <0 0 1> | <1 1 1> | 0.023 | 101.8 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 0.039 | 294.0 |
Au (mp-81) | <1 0 0> | <1 0 0> | 0.053 | 294.0 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 0.061 | 249.5 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 0.072 | 166.3 |
C (mp-48) | <0 0 1> | <1 0 0> | 0.081 | 294.0 |
NaCl (mp-22862) | <1 0 0> | <1 0 0> | 0.097 | 294.0 |
BN (mp-984) | <1 1 0> | <1 1 0> | 0.101 | 166.3 |
YAlO3 (mp-3792) | <1 0 1> | <1 0 0> | 0.107 | 294.0 |
Fe3O4 (mp-19306) | <1 0 0> | <1 0 0> | 0.121 | 294.0 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 0.125 | 294.0 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 0.131 | 249.5 |
SiC (mp-7631) | <1 0 0> | <1 0 0> | 0.159 | 235.2 |
PbSe (mp-2201) | <1 1 0> | <1 1 0> | 0.170 | 166.3 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 0.209 | 294.0 |
TbScO3 (mp-31119) | <0 0 1> | <1 1 0> | 0.224 | 249.5 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 0.250 | 249.5 |
GaSb (mp-1156) | <1 1 0> | <1 1 0> | 0.256 | 166.3 |
TiO2 (mp-390) | <1 0 0> | <1 0 0> | 0.289 | 294.0 |
TiO2 (mp-390) | <0 0 1> | <1 0 0> | 0.297 | 58.8 |
SiC (mp-7631) | <1 0 1> | <1 0 0> | 0.302 | 235.2 |
BN (mp-984) | <0 0 1> | <1 0 0> | 0.306 | 235.2 |
CdSe (mp-2691) | <1 1 0> | <1 1 0> | 0.338 | 166.3 |
Ge (mp-32) | <1 0 0> | <1 0 0> | 0.391 | 294.0 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 0.397 | 58.8 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 0.404 | 83.2 |
BN (mp-984) | <1 0 0> | <1 0 0> | 0.412 | 58.8 |
Si (mp-149) | <1 0 0> | <1 0 0> | 0.420 | 58.8 |
GaSe (mp-1943) | <0 0 1> | <1 1 0> | 0.426 | 249.5 |
Si (mp-149) | <1 1 0> | <1 1 0> | 0.428 | 83.2 |
Al (mp-134) | <1 1 0> | <1 1 0> | 0.428 | 249.5 |
TbScO3 (mp-31119) | <0 1 0> | <1 0 0> | 0.436 | 176.4 |
Te2Mo (mp-602) | <1 0 0> | <1 1 0> | 0.447 | 166.3 |
BN (mp-984) | <1 1 1> | <1 0 0> | 0.479 | 235.2 |
C (mp-48) | <1 0 0> | <1 1 0> | 0.490 | 249.5 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 0.506 | 176.4 |
C (mp-48) | <1 1 0> | <1 1 0> | 0.506 | 166.3 |
PbS (mp-21276) | <1 0 0> | <1 0 0> | 0.528 | 294.0 |
BaTiO3 (mp-5986) | <0 0 1> | <1 0 0> | 0.532 | 294.0 |
LiGaO2 (mp-5854) | <1 0 1> | <1 0 0> | 0.542 | 176.4 |
GdScO3 (mp-5690) | <0 1 0> | <1 0 0> | 0.572 | 176.4 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 0.615 | 294.0 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
316 | 165 | 165 | 0 | 0 | 0 |
165 | 316 | 165 | 0 | 0 | 0 |
165 | 165 | 316 | 0 | 0 | 0 |
0 | 0 | 0 | 95 | 0 | 0 |
0 | 0 | 0 | 0 | 95 | 0 |
0 | 0 | 0 | 0 | 0 | 95 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
4.9 | -1.7 | -1.7 | 0 | 0 | 0 |
-1.7 | 4.9 | -1.7 | 0 | 0 | 0 |
-1.7 | -1.7 | 4.9 | 0 | 0 | 0 |
0 | 0 | 0 | 10.5 | 0 | 0 |
0 | 0 | 0 | 0 | 10.5 | 0 |
0 | 0 | 0 | 0 | 0 | 10.5 |
Shear Modulus GV87 GPa |
Bulk Modulus KV215 GPa |
Shear Modulus GR86 GPa |
Bulk Modulus KR215 GPa |
Shear Modulus GVRH87 GPa |
Bulk Modulus KVRH215 GPa |
Elastic Anisotropy0.06 |
Poisson's Ratio0.32 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
YbNi4Au (mp-1024977) | 0.0000 | 0.040 | 3 |
TmInCu4 (mp-1024957) | 0.0028 | 0.000 | 3 |
GdNi4Au (mp-1077131) | 0.0027 | 0.855 | 3 |
YbCu4Au (mp-1077165) | 0.0028 | 0.000 | 3 |
GdInCu4 (mp-1077293) | 0.0009 | 0.000 | 3 |
AlFe2 (mp-31184) | 0.0000 | 0.137 | 2 |
PrMg2 (mp-30775) | 0.0000 | 0.014 | 2 |
CeFe2 (mp-204) | 0.0000 | 0.000 | 2 |
HoCo2 (mp-2396) | 0.0000 | 0.000 | 2 |
ZrFe2 (mp-1718) | 0.0000 | 0.000 | 2 |
Co (mp-1072089) | 0.0000 | 0.199 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Zr_sv W_pv |
Final Energy/Atom-11.6332 eV |
Corrected Energy-69.7995 eV
-69.7995 eV = -69.7995 eV (uncorrected energy)
|
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)