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-0.558 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. |
Density8.70 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 MauguinP62m [189] |
HallP 6 2 |
Point Group6m2 |
Crystal Systemhexagonal |
Topological ClassificationTI*
|
SubclassificationSEBR†
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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 |
---|---|---|---|
CaCdPb (mp-623089) | 0.1070 | 0.000 | 3 |
CaCdSn (mp-568695) | 0.0611 | 0.000 | 3 |
CaCdGe (mp-16258) | 0.0801 | 0.000 | 3 |
YbCdPb (mp-1080127) | 0.1227 | 0.000 | 3 |
YbCdSn (mp-1080680) | 0.0932 | 0.000 | 3 |
Yb3In3Ge2Au (mp-981207) | 0.1515 | 0.000 | 4 |
LiYb2InGe2 (mp-977355) | 0.4490 | 0.000 | 4 |
Sr2LiInGe2 (mp-571617) | 0.4593 | 0.000 | 4 |
LiCa2InGe2 (mp-570850) | 0.4500 | 0.000 | 4 |
U3Al3NiRu2 (mp-1080528) | 0.4643 | 0.087 | 4 |
Fe2P (mp-778) | 0.3186 | 0.000 | 2 |
BaCl2 (mp-567680) | 0.4358 | 0.030 | 2 |
Co2P (mp-13446) | 0.4745 | 0.022 | 2 |
TiO2 (mp-1079207) | 0.4761 | 0.326 | 2 |
Co2As (mp-1079254) | 0.4291 | 0.071 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Yb_2 Cd Ge_d |
Final Energy/Atom-2.9119 eV |
Corrected Energy-26.2075 eV
Uncorrected energy = -26.2075 eV
Corrected energy = -26.2075 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)