Final Magnetic Moment0.159 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-0.003 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.034 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. |
Density8.79 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCo2N + Cd + Co |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
C (mp-48) | <0 0 1> | <1 0 0> | 133.4 |
C (mp-48) | <1 0 0> | <1 1 0> | 167.8 |
LaAlO3 (mp-2920) | <1 0 0> | <1 1 0> | 146.8 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 74.1 |
LaAlO3 (mp-2920) | <1 1 1> | <1 1 1> | 128.4 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 104.8 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 29.7 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 41.9 |
CeO2 (mp-20194) | <1 1 1> | <1 1 0> | 251.6 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 133.4 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 167.8 |
SiO2 (mp-6930) | <1 0 0> | <1 1 0> | 83.9 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 167.8 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 0> | 222.4 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 74.1 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 133.4 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 188.7 |
ZnSe (mp-1190) | <1 1 1> | <1 1 1> | 179.8 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 133.4 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 222.4 |
InP (mp-20351) | <1 0 0> | <1 0 0> | 74.1 |
InP (mp-20351) | <1 1 1> | <1 1 1> | 179.8 |
C (mp-48) | <1 0 1> | <1 0 0> | 222.4 |
C (mp-48) | <1 1 0> | <1 1 0> | 167.8 |
C (mp-48) | <1 1 1> | <1 1 0> | 293.6 |
LaAlO3 (mp-2920) | <0 0 1> | <1 1 1> | 25.7 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 125.8 |
Te2W (mp-22693) | <1 0 0> | <1 1 0> | 293.6 |
CdWO4 (mp-19387) | <0 0 1> | <1 0 0> | 281.7 |
CdWO4 (mp-19387) | <0 1 0> | <1 0 0> | 133.4 |
CdWO4 (mp-19387) | <1 0 0> | <1 0 0> | 311.4 |
TePb (mp-19717) | <1 0 0> | <1 1 1> | 128.4 |
TePb (mp-19717) | <1 1 0> | <1 1 0> | 62.9 |
TePb (mp-19717) | <1 1 1> | <1 1 1> | 77.0 |
AlN (mp-661) | <0 0 1> | <1 1 1> | 25.7 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 163.1 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 83.9 |
AlN (mp-661) | <1 1 1> | <1 0 0> | 222.4 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 188.7 |
GaAs (mp-2534) | <1 1 1> | <1 1 1> | 179.8 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 192.8 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 333.9 |
SiO2 (mp-6930) | <1 1 0> | <1 1 0> | 188.7 |
Ni (mp-23) | <1 1 0> | <1 1 0> | 188.7 |
Ni (mp-23) | <1 1 1> | <1 1 1> | 333.9 |
BN (mp-984) | <0 0 1> | <1 1 0> | 83.9 |
BN (mp-984) | <1 0 1> | <1 0 0> | 192.8 |
BN (mp-984) | <1 1 0> | <1 1 0> | 167.8 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 192.8 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 62.9 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
316 | 122 | 122 | 0 | 0 | 0 |
122 | 316 | 122 | 0 | 0 | 0 |
122 | 122 | 316 | 0 | 0 | 0 |
0 | 0 | 0 | 87 | 0 | 0 |
0 | 0 | 0 | 0 | 87 | 0 |
0 | 0 | 0 | 0 | 0 | 87 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
4 | -1.1 | -1.1 | 0 | 0 | 0 |
-1.1 | 4 | -1.1 | 0 | 0 | 0 |
-1.1 | -1.1 | 4 | 0 | 0 | 0 |
0 | 0 | 0 | 11.5 | 0 | 0 |
0 | 0 | 0 | 0 | 11.5 | 0 |
0 | 0 | 0 | 0 | 0 | 11.5 |
Shear Modulus GV91 GPa |
Bulk Modulus KV186 GPa |
Shear Modulus GR91 GPa |
Bulk Modulus KR186 GPa |
Shear Modulus GVRH91 GPa |
Bulk Modulus KVRH186 GPa |
Elastic Anisotropy0.01 |
Poisson's Ratio0.29 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Pr3TlC (mp-7166) | 0.0000 | 1.823 | 3 |
Dy3TlC (mp-22513) | 0.0000 | 1.914 | 3 |
EuH3Pd (mp-644246) | 0.0000 | 0.000 | 3 |
ScPt3C (mp-1018628) | 0.0000 | 0.654 | 3 |
Pr3PbC (mp-20388) | 0.0000 | 1.886 | 3 |
Ba2VFeO6 (mp-1096778) | 0.0000 | 2.272 | 4 |
Ba2ScSbO6 (mp-20709) | 0.0000 | 2.196 | 4 |
Ba2YbSbO6 (mp-14223) | 0.0000 | 1.747 | 4 |
Ba2YSbO6 (mp-14226) | 0.0000 | 2.082 | 4 |
Ba2NbFeO6 (mp-1096853) | 0.0000 | 2.749 | 4 |
Ba3Sb2 (mp-1013582) | 0.0000 | 0.409 | 2 |
Mn4N (mp-505622) | 0.0000 | 0.000 | 2 |
Ba3P2 (mp-1013551) | 0.0000 | 0.446 | 2 |
Sr3Bi2 (mp-1013587) | 0.0000 | 0.373 | 2 |
Ca3As2 (mp-1096854) | 0.0000 | 0.360 | 2 |
BaLaMgBiO6 (mp-41414) | 0.0488 | 0.096 | 5 |
BaLaMgNbO6 (mp-39288) | 0.0712 | 0.090 | 5 |
SrLaNbZnO6 (mp-41918) | 0.0665 | 0.126 | 5 |
SrLaMnCoO6 (mp-40761) | 0.0404 | 0.247 | 5 |
Sr6Ca2MnFe7O24 (mp-1075969) | 0.0482 | 0.021 | 5 |
Na5Ca2Ce3Ti8Nb2O30 (mp-721094) | 0.7380 | 0.065 | 6 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Cd Co N |
Final Energy/Atom-6.0393 eV |
Corrected Energy-30.5577 eV
Uncorrected energy = -30.1967 eV
Composition-based energy adjustment (-0.361 eV/atom x 1.0 atoms) = -0.3610 eV
Corrected energy = -30.5577 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)