Final Magnetic Moment0.001 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 / Atom0.689 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.727 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. |
Density11.44 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToBi + NbMo |
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 MauguinF43m [216] |
HallF 4 2 3 |
Point Group43m |
Crystal Systemcubic |
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 | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 0 0> | 299.3 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 249.4 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 211.6 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 249.4 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 141.1 |
GaAs (mp-2534) | <1 1 1> | <1 1 0> | 282.1 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 199.5 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 211.6 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 259.2 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 86.4 |
SiO2 (mp-6930) | <1 1 1> | <1 1 0> | 211.6 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 199.5 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 282.1 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 211.6 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 249.4 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 199.5 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 211.6 |
InAs (mp-20305) | <1 1 1> | <1 1 1> | 259.2 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 249.4 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 141.1 |
ZnSe (mp-1190) | <1 1 1> | <1 1 0> | 282.1 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 70.5 |
KTaO3 (mp-3614) | <1 1 1> | <1 1 1> | 86.4 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 349.1 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 70.5 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 86.4 |
Te2W (mp-22693) | <0 0 1> | <1 1 0> | 282.1 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 49.9 |
YVO4 (mp-19133) | <1 0 1> | <1 0 0> | 199.5 |
YVO4 (mp-19133) | <1 1 1> | <1 0 0> | 249.4 |
Te2Mo (mp-602) | <0 0 1> | <1 0 0> | 349.1 |
Te2Mo (mp-602) | <1 0 0> | <1 1 0> | 211.6 |
Ag (mp-124) | <1 1 1> | <1 0 0> | 149.6 |
BN (mp-984) | <0 0 1> | <1 0 0> | 349.1 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 0 0> | 149.6 |
MoS2 (mp-1434) | <0 0 1> | <1 0 0> | 349.1 |
Al (mp-134) | <1 1 1> | <1 1 1> | 86.4 |
LiGaO2 (mp-5854) | <0 1 0> | <1 1 1> | 259.2 |
LiGaO2 (mp-5854) | <0 1 1> | <1 0 0> | 249.4 |
TeO2 (mp-2125) | <0 0 1> | <1 1 0> | 282.1 |
SiC (mp-7631) | <0 0 1> | <1 1 1> | 259.2 |
Fe3O4 (mp-19306) | <1 1 0> | <1 1 0> | 211.6 |
MgO (mp-1265) | <1 1 0> | <1 1 0> | 211.6 |
TiO2 (mp-2657) | <0 0 1> | <1 0 0> | 199.5 |
TiO2 (mp-2657) | <1 1 0> | <1 0 0> | 349.1 |
C (mp-66) | <1 1 1> | <1 0 0> | 349.1 |
GdScO3 (mp-5690) | <0 1 1> | <1 1 0> | 282.1 |
GdScO3 (mp-5690) | <1 0 1> | <1 1 1> | 172.8 |
LaF3 (mp-905) | <1 0 0> | <1 1 0> | 211.6 |
PbS (mp-21276) | <1 1 1> | <1 1 1> | 259.2 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
149 | 96 | 96 | 0 | 0 | 0 |
96 | 149 | 96 | 0 | 0 | 0 |
96 | 96 | 149 | 0 | 0 | 0 |
0 | 0 | 0 | -59 | 0 | 0 |
0 | 0 | 0 | 0 | -59 | 0 |
0 | 0 | 0 | 0 | 0 | -59 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
13.6 | -5.3 | -5.3 | 0 | 0 | 0 |
-5.3 | 13.6 | -5.3 | 0 | 0 | 0 |
-5.3 | -5.3 | 13.6 | 0 | 0 | 0 |
0 | 0 | 0 | -17.1 | 0 | 0 |
0 | 0 | 0 | 0 | -17.1 | 0 |
0 | 0 | 0 | 0 | 0 | -17.1 |
Shear Modulus GV-25 GPa |
Bulk Modulus KV114 GPa |
Shear Modulus GR205 GPa |
Bulk Modulus KR114 GPa |
Shear Modulus GVRH90 GPa |
Bulk Modulus KVRH114 GPa |
Elastic Anisotropy-5.60 |
Poisson's Ratio0.19 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
ScZn2Au (mp-972925) | 0.0000 | 0.019 | 3 |
LuScRu2 (mp-973433) | 0.0000 | 0.006 | 3 |
LiPm2Pt (mp-862842) | 0.0000 | 0.000 | 3 |
TmTc2W (mp-865250) | 0.0000 | 0.140 | 3 |
DyZnRh2 (mp-865257) | 0.0000 | 0.000 | 3 |
TiFeCoAs (mp-998974) | 0.0000 | 0.134 | 4 |
TiGaFeCo (mp-998964) | 0.0000 | 0.000 | 4 |
MnGaFeCo (mp-999552) | 0.0000 | 0.044 | 4 |
VGaFeCo (mp-1066581) | 0.0000 | 0.029 | 4 |
AlVFeCo (mp-1008530) | 0.0000 | 0.029 | 4 |
ZrSn3 (mp-1094224) | 0.0000 | 0.444 | 2 |
Mg3Al (mp-1094666) | 0.0000 | 0.075 | 2 |
Mg3Sn (mp-1094244) | 0.0000 | 0.090 | 2 |
Sm3V (mp-972456) | 0.0000 | 0.367 | 2 |
CrFe3 (mp-1018067) | 0.0000 | 0.064 | 2 |
Cu (mp-998890) | 0.0000 | 0.037 | 1 |
Kr (mp-974400) | 0.0000 | 0.002 | 1 |
H2 (mp-632250) | 0.0000 | 0.000 | 1 |
Ge (mp-998883) | 0.0000 | 0.339 | 1 |
U (mp-108) | 0.0000 | 0.269 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Nb_pv Bi Mo_pv |
Final Energy/Atom-6.4923 eV |
Corrected Energy-25.9692 eV
-25.9692 eV = -25.9692 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)