Final Magnetic Moment0.571 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-0.465 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. |
Density11.17 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 |
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] |
---|---|---|---|
KP(HO2)2 (mp-23959) | <0 0 1> | <1 0 0> | 235.9 |
MoSe2 (mp-1634) | <0 0 1> | <1 1 1> | 153.2 |
WSe2 (mp-1821) | <0 0 1> | <1 1 1> | 153.2 |
Ge (mp-32) | <1 0 0> | <1 0 0> | 265.4 |
Cu (mp-30) | <1 0 0> | <1 0 0> | 117.9 |
Cu (mp-30) | <1 1 0> | <1 1 0> | 166.8 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 153.2 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 265.4 |
Al (mp-134) | <1 0 0> | <1 0 0> | 147.4 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 166.8 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 204.3 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 125.1 |
InSb (mp-20012) | <1 1 0> | <1 1 0> | 125.1 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 265.4 |
MgAl2O4 (mp-3536) | <1 0 0> | <1 0 0> | 265.4 |
CdTe (mp-406) | <1 1 0> | <1 1 0> | 125.1 |
C (mp-48) | <0 0 1> | <1 1 1> | 204.3 |
Fe2O3 (mp-24972) | <0 0 1> | <1 1 1> | 204.3 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 1 1> | 51.1 |
LiGaO2 (mp-5854) | <0 0 1> | <1 1 0> | 83.4 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 147.4 |
Ni (mp-23) | <1 1 0> | <1 1 0> | 333.6 |
YAlO3 (mp-3792) | <1 0 1> | <1 0 0> | 147.4 |
TbScO3 (mp-31119) | <0 0 1> | <1 1 0> | 125.1 |
CaCO3 (mp-3953) | <0 0 1> | <1 1 1> | 153.2 |
LiGaO2 (mp-5854) | <1 0 0> | <1 0 0> | 176.9 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 250.2 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 204.3 |
MgF2 (mp-1249) | <1 0 0> | <1 1 0> | 291.9 |
C (mp-66) | <1 1 1> | <1 1 1> | 153.2 |
GaSe (mp-1943) | <0 0 1> | <1 1 1> | 51.1 |
SiC (mp-7631) | <1 0 1> | <1 0 0> | 235.9 |
Fe3O4 (mp-19306) | <1 0 0> | <1 0 0> | 147.4 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 125.1 |
SiC (mp-7631) | <1 0 0> | <1 0 0> | 235.9 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 324.3 |
SiC (mp-8062) | <1 1 1> | <1 1 0> | 166.8 |
PbSe (mp-2201) | <1 1 0> | <1 1 0> | 166.8 |
PbSe (mp-2201) | <1 1 1> | <1 1 1> | 204.3 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 29.5 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 41.7 |
CeO2 (mp-20194) | <1 1 1> | <1 1 1> | 51.1 |
TeO2 (mp-2125) | <1 1 0> | <1 0 0> | 294.8 |
Si (mp-149) | <1 0 0> | <1 0 0> | 29.5 |
Si (mp-149) | <1 1 0> | <1 1 0> | 41.7 |
Al (mp-134) | <1 1 0> | <1 1 0> | 250.2 |
Si (mp-149) | <1 1 1> | <1 1 1> | 51.1 |
TiO2 (mp-390) | <1 1 1> | <1 0 0> | 324.3 |
ZrO2 (mp-2858) | <1 1 0> | <1 0 0> | 324.3 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 265.4 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
356 | 149 | 149 | 0 | 0 | 0 |
149 | 356 | 149 | 0 | 0 | 0 |
149 | 149 | 356 | 0 | 0 | 0 |
0 | 0 | 0 | 117 | 0 | 0 |
0 | 0 | 0 | 0 | 117 | 0 |
0 | 0 | 0 | 0 | 0 | 117 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
3.7 | -1.1 | -1.1 | 0 | 0 | 0 |
-1.1 | 3.7 | -1.1 | 0 | 0 | 0 |
-1.1 | -1.1 | 3.7 | 0 | 0 | 0 |
0 | 0 | 0 | 8.5 | 0 | 0 |
0 | 0 | 0 | 0 | 8.5 | 0 |
0 | 0 | 0 | 0 | 0 | 8.5 |
Shear Modulus GV112 GPa |
Bulk Modulus KV218 GPa |
Shear Modulus GR111 GPa |
Bulk Modulus KR218 GPa |
Shear Modulus GVRH111 GPa |
Bulk Modulus KVRH218 GPa |
Elastic Anisotropy0.02 |
Poisson's Ratio0.28 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
YHoAg2 (mp-979425) | 0.0000 | 0.000 | 3 |
SmSnPd2 (mp-978538) | 0.0000 | 0.002 | 3 |
LiPm2Al (mp-861948) | 0.0000 | 0.000 | 3 |
Na2TlBi (mp-864898) | 0.0000 | 0.000 | 3 |
Tb2IrRh (mp-867282) | 0.0000 | 0.000 | 3 |
LiMgSnPd (mp-7555) | 0.0000 | 0.000 | 4 |
LiMgSnAu (mp-7554) | 0.0000 | 0.058 | 4 |
LiMgSbPt (mp-571584) | 0.0000 | 0.086 | 4 |
LiMgSbPd (mp-10179) | 0.0000 | 0.074 | 4 |
LiMgSnPt (mp-11806) | 0.0000 | 0.000 | 4 |
Tl3Zn (mp-981380) | 0.0000 | 0.131 | 2 |
TmO3 (mp-979074) | 0.0000 | 0.559 | 2 |
SnBi3 (mp-978882) | 0.0000 | 0.107 | 2 |
SnAs3 (mp-978881) | 0.0000 | 0.392 | 2 |
V3Ru (mp-865382) | 0.0000 | 0.000 | 2 |
Br (mp-673171) | 0.0000 | 0.630 | 1 |
Ti (mp-73) | 0.0000 | 0.112 | 1 |
I (mp-684663) | 0.0000 | 0.446 | 1 |
Cr (mp-90) | 0.0000 | 0.000 | 1 |
Bi (mp-568610) | 0.0000 | 0.139 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Be_sv Co Ir |
Final Energy/Atom-6.3215 eV |
Corrected Energy-25.2861 eV
-25.2861 eV = -25.2861 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)