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-0.359 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. |
Density9.74 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†
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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.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 0 0> | 340.6 |
AlN (mp-661) | <1 0 0> | <1 1 1> | 252.8 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 243.3 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 137.6 |
GaAs (mp-2534) | <1 1 1> | <1 1 0> | 275.3 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 194.6 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 243.3 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 340.6 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 340.6 |
SiO2 (mp-6930) | <1 1 1> | <1 1 0> | 206.4 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 194.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 275.3 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 275.3 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 1> | 168.6 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 243.3 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 194.6 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 206.4 |
InAs (mp-20305) | <1 1 1> | <1 1 1> | 252.8 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 137.6 |
ZnSe (mp-1190) | <1 1 1> | <1 1 0> | 275.3 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 68.8 |
KTaO3 (mp-3614) | <1 1 1> | <1 1 1> | 84.3 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 146.0 |
CdS (mp-672) | <1 1 0> | <1 1 0> | 206.4 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 68.8 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 84.3 |
Ag (mp-124) | <1 1 0> | <1 1 0> | 275.3 |
Fe3O4 (mp-19306) | <1 1 0> | <1 1 0> | 206.4 |
MgO (mp-1265) | <1 1 0> | <1 1 0> | 206.4 |
TiO2 (mp-2657) | <0 0 1> | <1 0 0> | 194.6 |
TiO2 (mp-2657) | <1 0 0> | <1 0 0> | 340.6 |
C (mp-66) | <1 1 0> | <1 1 1> | 252.8 |
C (mp-66) | <1 1 1> | <1 0 0> | 340.6 |
GdScO3 (mp-5690) | <1 0 1> | <1 1 1> | 168.6 |
KP(HO2)2 (mp-23959) | <0 0 1> | <1 0 0> | 146.0 |
Al (mp-134) | <1 1 0> | <1 1 0> | 68.8 |
Al (mp-134) | <1 1 1> | <1 1 1> | 84.3 |
KP(HO2)2 (mp-23959) | <0 1 1> | <1 1 0> | 206.4 |
InP (mp-20351) | <1 1 1> | <1 1 1> | 252.8 |
TbScO3 (mp-31119) | <0 0 1> | <1 1 0> | 275.3 |
TbScO3 (mp-31119) | <1 0 1> | <1 1 1> | 168.6 |
TbScO3 (mp-31119) | <1 1 0> | <1 0 0> | 243.3 |
SiC (mp-7631) | <0 0 1> | <1 0 0> | 292.0 |
Ni (mp-23) | <1 1 1> | <1 1 1> | 84.3 |
PbSe (mp-2201) | <1 0 0> | <1 0 0> | 194.6 |
NdGaO3 (mp-3196) | <0 0 1> | <1 1 0> | 275.3 |
NdGaO3 (mp-3196) | <1 1 0> | <1 0 0> | 243.3 |
MgO (mp-1265) | <1 0 0> | <1 0 0> | 243.3 |
C (mp-66) | <1 0 0> | <1 1 1> | 252.8 |
GdScO3 (mp-5690) | <0 1 1> | <1 1 0> | 275.3 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
86 | 76 | 76 | 0 | 0 | 0 |
76 | 86 | 76 | 0 | 0 | 0 |
76 | 76 | 86 | 0 | 0 | 0 |
0 | 0 | 0 | 43 | 0 | 0 |
0 | 0 | 0 | 0 | 43 | 0 |
0 | 0 | 0 | 0 | 0 | 43 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
68 | -31.9 | -31.9 | 0 | 0 | 0 |
-31.9 | 68 | -31.9 | 0 | 0 | 0 |
-31.9 | -31.9 | 68 | 0 | 0 | 0 |
0 | 0 | 0 | 23.5 | 0 | 0 |
0 | 0 | 0 | 0 | 23.5 | 0 |
0 | 0 | 0 | 0 | 0 | 23.5 |
Shear Modulus GV28 GPa |
Bulk Modulus KV79 GPa |
Shear Modulus GR11 GPa |
Bulk Modulus KR79 GPa |
Shear Modulus GVRH19 GPa |
Bulk Modulus KVRH79 GPa |
Elastic Anisotropy7.95 |
Poisson's Ratio0.39 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Li2GaIr (mp-31441) | 0.0000 | 0.000 | 3 |
TaGaCo2 (mp-30555) | 0.0000 | 0.000 | 3 |
AlVFe2 (mp-5778) | 0.0000 | 0.000 | 3 |
ScInPd2 (mp-31339) | 0.0000 | 0.000 | 3 |
NbCo2Sn (mp-4583) | 0.0000 | 0.119 | 3 |
LiMgSnPd (mp-7555) | 0.0000 | 0.000 | 4 |
VFeCoGe (mp-1063914) | 0.0000 | 0.000 | 4 |
TiFeCoGe (mp-1018012) | 0.0000 | 0.028 | 4 |
VGaFeCo (mp-1066581) | 0.0000 | 0.029 | 4 |
LiMgSbPd (mp-10179) | 0.0000 | 0.074 | 4 |
Rb3Bi (mp-23304) | 0.0000 | 0.028 | 2 |
LaMg3 (mp-2306) | 0.0000 | 0.063 | 2 |
LiGa (mp-1307) | 0.0000 | 0.000 | 2 |
Li3Hg (mp-1646) | 0.0000 | 0.000 | 2 |
NaTl (mp-1564) | 0.0000 | 0.000 | 2 |
Eu (mp-20071) | 0.0000 | 0.083 | 1 |
Ba (mp-122) | 0.0000 | 0.000 | 1 |
Ce (mp-10024) | 0.0000 | 0.228 | 1 |
Np (mp-10207) | 0.0000 | 0.447 | 1 |
Gd (mp-11421) | 0.0000 | 0.088 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Er_3 In_d Ag |
Final Energy/Atom-3.6048 eV |
Corrected Energy-14.4194 eV
-14.4194 eV = -14.4194 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)