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-0.424 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. |
Density8.90 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 MauguinCmcm [63] |
Hall-C 2c 2 |
Point Groupmmm |
Crystal Systemorthorhombic |
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 |
---|---|---|---|
TbIn2Ni (mp-672325) | 0.1287 | 0.000 | 3 |
LuAl2Ni (mp-1025389) | 0.2112 | 0.000 | 3 |
YIn2Ni (mp-22056) | 0.1619 | 0.000 | 3 |
CaSn2Ir (mp-11957) | 0.2100 | 0.000 | 3 |
CaIn2Cu (mp-19968) | 0.1747 | 0.012 | 3 |
Na2LiGaAs2 (mp-9722) | 0.7164 | 0.000 | 4 |
LiYb2InGe2 (mp-977355) | 0.7043 | 0.000 | 4 |
Sr2LiInGe2 (mp-571617) | 0.7164 | 0.000 | 4 |
LiCa2InGe2 (mp-570850) | 0.6962 | 0.000 | 4 |
MgH2 (mp-23712) | 0.5568 | 0.082 | 2 |
YbF3 (mp-22072) | 0.6038 | 0.000 | 2 |
KGe (mp-2146) | 0.6411 | 0.041 | 2 |
CsSn (mp-571056) | 0.6247 | 0.000 | 2 |
EuF3 (mp-19908) | 0.6462 | 0.206 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Dy_3 In_d Ni_pv |
Final Energy/Atom-4.3969 eV |
Corrected Energy-35.1750 eV
Uncorrected energy = -35.1750 eV
Corrected energy = -35.1750 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)