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-0.563 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. |
Density10.32 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 MauguinP63mc [186] |
HallP 6c 2c |
Point Group6mm |
Crystal Systemhexagonal |
Topological ClassificationSM*
|
SubclassificationES†
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Crossing TypeLine
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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 |
---|---|---|---|
CaAgBi (mp-568664) | 0.0819 | 0.000 | 3 |
CaSnHg (mp-1019104) | 0.0639 | 0.000 | 3 |
EuHgPb (mp-1018698) | 0.0980 | 0.000 | 3 |
YbZnPb (mp-1077097) | 0.0697 | 0.000 | 3 |
ErAgSn (mp-569724) | 0.1057 | 0.000 | 3 |
LiTb(CuP)2 (mp-8220) | 0.7180 | 0.000 | 4 |
LiSm(CuP)2 (mp-973019) | 0.6863 | 0.000 | 4 |
LiYb(CuP)2 (mp-1024988) | 0.6926 | 0.000 | 4 |
LiY(CuP)2 (mp-1018791) | 0.7179 | 0.000 | 4 |
LiCe(CuP)2 (mp-1018784) | 0.7219 | 0.000 | 4 |
EuTl2 (mp-30630) | 0.2022 | 0.000 | 2 |
MgGa2 (mp-30651) | 0.2687 | 0.005 | 2 |
EuIn2 (mp-636316) | 0.2277 | 0.000 | 2 |
YbIn2 (mp-568058) | 0.2129 | 0.000 | 2 |
CaIn2 (mp-21068) | 0.1889 | 0.000 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Yb_2 Sn_d Hg |
Final Energy/Atom-2.5137 eV |
Corrected Energy-15.0824 eV
-15.0824 eV = -15.0824 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)