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-0.835 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. |
Density10.53 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 MauguinPm3m [221] |
Hall-P 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.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 1 0> | 171.7 |
AlN (mp-661) | <1 0 0> | <1 1 0> | 220.8 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 122.6 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 220.8 |
AlN (mp-661) | <1 1 1> | <1 1 0> | 196.2 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 156.1 |
CeO2 (mp-20194) | <1 1 1> | <1 1 1> | 210.3 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 34.7 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 49.1 |
GaAs (mp-2534) | <1 1 1> | <1 0 0> | 173.4 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 156.1 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 220.8 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 210.3 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 242.8 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 260.2 |
GaN (mp-804) | <1 0 1> | <1 1 0> | 171.7 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 220.8 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 277.5 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 90.1 |
SiO2 (mp-6930) | <1 0 0> | <1 1 0> | 220.8 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 269.8 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 86.7 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 220.8 |
KCl (mp-23193) | <1 1 1> | <1 1 1> | 210.3 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 98.1 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 138.8 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 0> | 171.7 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 312.2 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 156.1 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 220.8 |
InAs (mp-20305) | <1 1 1> | <1 1 1> | 210.3 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 34.7 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 49.1 |
ZnSe (mp-1190) | <1 1 1> | <1 0 0> | 173.4 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 138.8 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 196.2 |
CdS (mp-672) | <0 0 1> | <1 0 0> | 121.4 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 86.7 |
CdS (mp-672) | <1 0 1> | <1 0 0> | 190.8 |
CdS (mp-672) | <1 1 0> | <1 1 1> | 360.5 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 17.3 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 24.5 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 30.0 |
Te2W (mp-22693) | <0 0 1> | <1 1 0> | 196.2 |
Te2W (mp-22693) | <0 1 0> | <1 1 0> | 318.9 |
Te2W (mp-22693) | <0 1 1> | <1 1 0> | 171.7 |
Te2W (mp-22693) | <1 1 0> | <1 1 0> | 220.8 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 277.5 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 260.2 |
TePb (mp-19717) | <1 0 0> | <1 0 0> | 86.7 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
202 | 92 | 92 | 0 | 0 | 0 |
92 | 202 | 92 | 0 | 0 | 0 |
92 | 92 | 202 | 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) |
|||||
---|---|---|---|---|---|
6.9 | -2.2 | -2.2 | 0 | 0 | 0 |
-2.2 | 6.9 | -2.2 | 0 | 0 | 0 |
-2.2 | -2.2 | 6.9 | 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 GV57 GPa |
Bulk Modulus KV129 GPa |
Shear Modulus GR57 GPa |
Bulk Modulus KR129 GPa |
Shear Modulus GVRH57 GPa |
Bulk Modulus KVRH129 GPa |
Elastic Anisotropy0.01 |
Poisson's Ratio0.31 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
ZnCu2Ni (mp-30593) | 0.1125 | 0.005 | 3 |
CrCoPt2 (mp-570863) | 0.0492 | 0.000 | 3 |
LiCa6Ge (mp-12609) | 0.0000 | 0.180 | 3 |
GaFeNi2 (mp-1065359) | 0.0412 | 0.066 | 3 |
GaCo2Ni (mp-1018060) | 0.0157 | 0.075 | 3 |
Cr8Ni50Mo15W2 (mp-767372) | 0.2155 | 0.028 | 4 |
CrFeCoNi (mp-1012640) | 0.3608 | 0.118 | 4 |
CrFeCoNi (mp-1096923) | 0.4019 | 0.193 | 4 |
DyIn3 (mp-20236) | 0.0000 | 0.000 | 2 |
TbPd3 (mp-2747) | 0.0000 | 0.000 | 2 |
YbAl3 (mp-1259) | 0.0000 | 0.103 | 2 |
Ce3Al (mp-2413) | 0.0000 | 0.016 | 2 |
TmIn3 (mp-21177) | 0.0000 | 0.000 | 2 |
Na (mp-974558) | 0.0000 | 0.001 | 1 |
Br (mp-998870) | 0.0000 | 0.666 | 1 |
Mn (mp-8634) | 0.0000 | 0.083 | 1 |
Pb (mp-20483) | 0.0000 | 0.000 | 1 |
Cu (mp-30) | 0.0000 | 0.000 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ce Pd |
Final Energy/Atom-6.2004 eV |
Corrected Energy-24.8015 eV
Uncorrected energy = -24.8015 eV
Corrected energy = -24.8015 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)