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-0.050 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. |
Density8.85 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†
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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] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 224.2 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 129.7 |
AlN (mp-661) | <0 0 1> | <1 0 0> | 51.0 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 71.3 |
AlN (mp-661) | <1 1 1> | <1 1 1> | 229.5 |
CeO2 (mp-20194) | <1 0 0> | <1 1 1> | 88.3 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 43.2 |
CeO2 (mp-20194) | <1 1 1> | <1 1 1> | 53.0 |
LaAlO3 (mp-2920) | <0 0 1> | <1 0 0> | 224.2 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 81.5 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 158.6 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 132.5 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 273.9 |
GaAs (mp-2534) | <1 1 1> | <1 1 1> | 229.5 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 40.8 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 57.7 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 70.6 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 51.0 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 71.3 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 112.1 |
GaN (mp-804) | <1 1 0> | <1 1 1> | 300.1 |
GaN (mp-804) | <1 1 1> | <1 1 0> | 302.7 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 158.9 |
SiO2 (mp-6930) | <1 0 0> | <1 0 0> | 193.7 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 273.9 |
SiO2 (mp-6930) | <1 1 0> | <1 1 0> | 345.9 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 57.7 |
KCl (mp-23193) | <1 1 1> | <1 1 1> | 70.6 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 40.8 |
DyScO3 (mp-31120) | <0 1 0> | <1 1 0> | 43.2 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 214.0 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 91.7 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 0> | 214.0 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 129.7 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 132.5 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 0> | 275.2 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 158.6 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 183.5 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 132.5 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 273.9 |
ZnSe (mp-1190) | <1 1 1> | <1 1 1> | 229.5 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 81.5 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 254.8 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 245.0 |
CdS (mp-672) | <1 0 1> | <1 1 0> | 158.6 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 81.5 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 245.0 |
CdS (mp-672) | <0 0 1> | <1 1 0> | 230.6 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 265.0 |
CdS (mp-672) | <1 1 0> | <1 0 0> | 316.0 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
97 | 88 | 88 | 0 | 0 | 0 |
88 | 97 | 88 | 0 | 0 | 0 |
88 | 88 | 97 | 0 | 0 | 0 |
0 | 0 | 0 | 55 | 0 | 0 |
0 | 0 | 0 | 0 | 55 | 0 |
0 | 0 | 0 | 0 | 0 | 55 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
71.1 | -33.7 | -33.7 | 0 | 0 | 0 |
-33.7 | 71.1 | -33.7 | 0 | 0 | 0 |
-33.7 | -33.7 | 71.1 | 0 | 0 | 0 |
0 | 0 | 0 | 18.3 | 0 | 0 |
0 | 0 | 0 | 0 | 18.3 | 0 |
0 | 0 | 0 | 0 | 0 | 18.3 |
Shear Modulus GV35 GPa |
Bulk Modulus KV91 GPa |
Shear Modulus GR11 GPa |
Bulk Modulus KR91 GPa |
Shear Modulus GVRH23 GPa |
Bulk Modulus KVRH91 GPa |
Elastic Anisotropy11.43 |
Poisson's Ratio0.39 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
HoTmZn2 (mp-983126) | 0.0000 | 0.000 | 3 |
Pm2PtAu (mp-982772) | 0.0000 | 0.000 | 3 |
Nd2IrAu (mp-973606) | 0.0000 | 0.057 | 3 |
YbPrPd2 (mp-981530) | 0.0000 | 0.011 | 3 |
YTmAl2 (mp-980662) | 0.0000 | 0.016 | 3 |
TiFeCoSb (mp-998973) | 0.0000 | 0.186 | 4 |
TiAlFeCo (mp-998980) | 0.0000 | 0.000 | 4 |
TiFeCoGe (mp-1018012) | 0.0000 | 0.028 | 4 |
VFeCoSi (mp-1066609) | 0.0000 | 0.002 | 4 |
VFeCoSb (mp-1066862) | 0.0000 | 0.163 | 4 |
ErPd (mp-851) | 0.0000 | 0.000 | 2 |
YbRu (mp-567116) | 0.0000 | 0.209 | 2 |
PrIn (mp-20023) | 0.0000 | 0.000 | 2 |
ReC (mp-1009731) | 0.0000 | 1.115 | 2 |
ScCu (mp-1169) | 0.0000 | 0.000 | 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: Zn Ag |
Final Energy/Atom-2.0958 eV |
Corrected Energy-4.1915 eV
-4.1915 eV = -4.1915 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)