Final Magnetic Moment0.003 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-0.406 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. |
Density8.54 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 MauguinFm3m [225] |
Hall-F 4 2 3 |
Point Groupm3m |
Crystal Systemcubic |
Topological ClassificationSM*
|
SubclassificationESFD†
|
Crossing TypePoint
|
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.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
CeO2 (mp-20194) | <1 1 1> | <1 1 1> | 207.1 |
AlN (mp-661) | <0 0 1> | <1 1 0> | 169.1 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 279.0 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 281.9 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 169.1 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 39.9 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 69.0 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 159.4 |
SiO2 (mp-6930) | <1 1 0> | <1 0 0> | 239.2 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 159.4 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 56.4 |
GaN (mp-804) | <0 0 1> | <1 1 1> | 276.2 |
GaN (mp-804) | <1 0 0> | <1 1 0> | 169.1 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 199.3 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 56.4 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 338.2 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 318.9 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 39.9 |
InAs (mp-20305) | <1 1 1> | <1 1 1> | 69.0 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 159.4 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 39.9 |
KCl (mp-23193) | <1 1 1> | <1 1 1> | 69.0 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 56.4 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 79.7 |
CdS (mp-672) | <0 0 1> | <1 1 0> | 225.5 |
Te2W (mp-22693) | <0 0 1> | <1 1 0> | 112.7 |
Te2W (mp-22693) | <1 0 0> | <1 0 0> | 199.3 |
Te2W (mp-22693) | <1 0 1> | <1 0 0> | 199.3 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 199.3 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 207.1 |
Te2W (mp-22693) | <0 1 0> | <1 1 1> | 276.2 |
YVO4 (mp-19133) | <1 0 0> | <1 1 0> | 225.5 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 199.3 |
TePb (mp-19717) | <1 0 0> | <1 0 0> | 358.8 |
Te2Mo (mp-602) | <0 0 1> | <1 0 0> | 199.3 |
Te2Mo (mp-602) | <1 0 0> | <1 1 1> | 276.2 |
Te2Mo (mp-602) | <1 0 1> | <1 1 1> | 276.2 |
Te2Mo (mp-602) | <1 1 0> | <1 0 0> | 199.3 |
Te2Mo (mp-602) | <1 1 1> | <1 0 0> | 199.3 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 159.4 |
Ag (mp-124) | <1 1 0> | <1 1 0> | 225.5 |
Ag (mp-124) | <1 1 1> | <1 1 1> | 207.1 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 1 1> | 69.0 |
BN (mp-984) | <1 0 1> | <1 1 0> | 338.2 |
BN (mp-984) | <1 1 1> | <1 0 0> | 279.0 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 0> | 225.5 |
BN (mp-984) | <0 0 1> | <1 1 0> | 225.5 |
BN (mp-984) | <1 1 0> | <1 1 1> | 69.0 |
LiNbO3 (mp-3731) | <0 0 1> | <1 1 1> | 69.0 |
MoS2 (mp-1434) | <0 0 1> | <1 1 1> | 276.2 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
185 | 117 | 117 | 0 | 0 | 0 |
117 | 185 | 117 | 0 | 0 | 0 |
117 | 117 | 185 | 0 | 0 | 0 |
0 | 0 | 0 | 67 | 0 | 0 |
0 | 0 | 0 | 0 | 67 | 0 |
0 | 0 | 0 | 0 | 0 | 67 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
10.6 | -4.1 | -4.1 | 0 | 0 | 0 |
-4.1 | 10.6 | -4.1 | 0 | 0 | 0 |
-4.1 | -4.1 | 10.6 | 0 | 0 | 0 |
0 | 0 | 0 | 14.8 | 0 | 0 |
0 | 0 | 0 | 0 | 14.8 | 0 |
0 | 0 | 0 | 0 | 0 | 14.8 |
Shear Modulus GV54 GPa |
Bulk Modulus KV139 GPa |
Shear Modulus GR48 GPa |
Bulk Modulus KR139 GPa |
Shear Modulus GVRH51 GPa |
Bulk Modulus KVRH139 GPa |
Elastic Anisotropy0.58 |
Poisson's Ratio0.34 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
LiAg2Ge (mp-9472) | 0.0000 | 0.005 | 3 |
TiAlNi2 (mp-7187) | 0.0000 | 0.000 | 3 |
TbSnPd2 (mp-5385) | 0.0000 | 0.000 | 3 |
MnCo2Sb (mp-5396) | 0.0000 | 0.000 | 3 |
TiFe2Sn (mp-19963) | 0.0000 | 0.000 | 3 |
LiMgSnPd (mp-7555) | 0.0000 | 0.000 | 4 |
LiMgSnAu (mp-7554) | 0.0000 | 0.088 | 4 |
VFeCoGe (mp-1063914) | 0.0000 | 0.000 | 4 |
LiMgSbPd (mp-10179) | 0.0000 | 0.096 | 4 |
LiMgSnPt (mp-11806) | 0.0000 | 0.000 | 4 |
Mn3Si (mp-20211) | 0.0000 | 0.000 | 2 |
NaIn (mp-20628) | 0.0000 | 0.000 | 2 |
NdMg3 (mp-1787) | 0.0000 | 0.000 | 2 |
AlFe3 (mp-2018) | 0.0000 | 0.004 | 2 |
K3Sb (mp-10159) | 0.0000 | 0.028 | 2 |
Sr (mp-95) | 0.0000 | 0.013 | 1 |
Yb (mp-71) | 0.0000 | 0.017 | 1 |
Fe (mp-13) | 0.0000 | 0.000 | 1 |
Nb (mp-75) | 0.0000 | 0.000 | 1 |
Li (mp-135) | 0.0000 | 0.005 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Zr_sv In_d Ni_pv |
Final Energy/Atom-6.1206 eV |
Corrected Energy-24.4825 eV
Uncorrected energy = -24.4825 eV
Corrected energy = -24.4825 eV
|
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)