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-0.002 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.107 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. |
Density5.01 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToMgCd |
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 MauguinP6m2 [187] |
HallP 6 2 |
Point Group6m2 |
Crystal Systemhexagonal |
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> | <0 0 1> | 35.6 |
C (mp-48) | <1 0 0> | <0 0 1> | 177.9 |
C (mp-48) | <1 0 1> | <0 0 1> | 177.9 |
C (mp-48) | <1 1 1> | <0 0 1> | 204.6 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 26.7 |
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 71.2 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 80.0 |
LaAlO3 (mp-2920) | <1 1 1> | <0 0 1> | 133.4 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 8.9 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 48.4 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 145.1 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 83.8 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 204.6 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 88.9 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 83.8 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 169.0 |
BaF2 (mp-1029) | <1 0 0> | <1 0 1> | 196.8 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 167.6 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 275.7 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 62.3 |
SiO2 (mp-6930) | <1 0 0> | <1 1 0> | 83.8 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 311.3 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 142.3 |
SiO2 (mp-6930) | <1 1 1> | <0 0 1> | 311.3 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 284.6 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 177.9 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 222.4 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 160.1 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 302.4 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 53.4 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 320.2 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 311.3 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 275.7 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 169.0 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 80.0 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 160.1 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 26.7 |
InP (mp-20351) | <1 0 0> | <0 0 1> | 346.9 |
InP (mp-20351) | <1 1 0> | <0 0 1> | 249.0 |
InP (mp-20351) | <1 1 1> | <0 0 1> | 62.3 |
Te2W (mp-22693) | <0 0 1> | <1 0 1> | 196.8 |
Te2W (mp-22693) | <1 0 0> | <1 0 0> | 96.8 |
CdWO4 (mp-19387) | <0 0 1> | <0 0 1> | 275.7 |
CdWO4 (mp-19387) | <0 1 0> | <0 0 1> | 204.6 |
CdWO4 (mp-19387) | <0 1 1> | <0 0 1> | 284.6 |
CdWO4 (mp-19387) | <1 0 0> | <1 1 0> | 251.4 |
CdWO4 (mp-19387) | <1 1 0> | <1 0 1> | 245.9 |
CdWO4 (mp-19387) | <1 1 1> | <0 0 1> | 249.0 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 213.5 |
TePb (mp-19717) | <1 1 0> | <0 0 1> | 177.9 |
A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Cr8Ni50Mo15W2 (mp-767372) | 0.2712 | 0.028 | 4 |
CrFeCoNi (mp-1012640) | 0.1235 | 0.118 | 4 |
CrFeCoNi (mp-1096923) | 0.3560 | 0.193 | 4 |
Y2Mg (mp-1094423) | 0.0345 | 0.133 | 2 |
LiMg2 (mp-1094581) | 0.0344 | 0.035 | 2 |
Li5Mg (mp-1094590) | 0.0356 | 0.018 | 2 |
LiMg (mp-1094592) | 0.0416 | 0.043 | 2 |
Mg2Cd (mp-1039309) | 0.0322 | 0.104 | 2 |
Pr (mp-1059256) | 0.0832 | 0.029 | 1 |
Ru (mp-33) | 0.0900 | 0.000 | 1 |
Os (mp-49) | 0.0909 | 0.000 | 1 |
Tb (mp-18) | 0.0889 | 0.019 | 1 |
Sc (mp-67) | 0.0836 | 0.000 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv Cd |
Final Energy/Atom-1.2534 eV |
Corrected Energy-7.5206 eV
Uncorrected energy = -7.5206 eV
Corrected energy = -7.5206 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)