Final Magnetic Moment0.678 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 / Atom0.207 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.207 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. |
Density2.30 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToK + Pd |
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 |
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%)
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 |
---|---|---|---|
ZnCu2Ni (mp-30593) | 0.1125 | 0.005 | 3 |
CrCoPt2 (mp-570863) | 0.0492 | 0.034 | 3 |
LiCa6Ge (mp-12609) | 0.0000 | 0.183 | 3 |
GaFeNi2 (mp-1065359) | 0.0412 | 0.065 | 3 |
GaCo2Ni (mp-1018060) | 0.0157 | 0.075 | 3 |
Cr8Ni50Mo15W2 (mp-767372) | 0.2155 | 0.028 | 4 |
CrFeCoNi (mp-1012640) | 0.3608 | 0.065 | 4 |
CrFeCoNi (mp-1096923) | 0.4019 | 0.193 | 4 |
GdTl3 (mp-20503) | 0.0000 | 0.000 | 2 |
Mg7Nb (mp-1079163) | 0.0000 | 0.127 | 2 |
HoPd3 (mp-1979) | 0.0000 | 0.000 | 2 |
ScPd3 (mp-2677) | 0.0000 | 0.000 | 2 |
Sm3Ga (mp-1066795) | 0.0000 | 0.074 | 2 |
H2 (mp-634659) | 0.0000 | 0.000 | 1 |
Sr (mp-76) | 0.0000 | 0.006 | 1 |
Ni (mp-1056486) | 0.0000 | 0.000 | 1 |
Cd (mp-1096861) | 0.0000 | 0.000 | 1 |
Pd (mp-1056438) | 0.0000 | 0.000 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: K_sv Pd |
Final Energy/Atom-1.9210 eV |
Corrected Energy-7.6838 eV
-7.6838 eV = -7.6838 eV (uncorrected energy)
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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)