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-0.824 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. |
Density11.71 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 MauguinPnma [62] |
Hall-P 2ac 2n |
Point Groupmmm |
Crystal Systemorthorhombic |
Topological ClassificationSM*
|
SubclassificationES†
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Crossing TypePlane
|
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 |
---|---|---|---|
NbCoP (mp-21449) | 0.0743 | 0.000 | 3 |
CaInRh (mp-20220) | 0.1379 | 0.000 | 3 |
NbSiRh (mp-10470) | 0.1698 | 0.000 | 3 |
NbSiIr (mp-21248) | 0.1660 | 0.000 | 3 |
TaMnP (mp-21066) | 0.1762 | 0.000 | 3 |
Na2LiGaAs2 (mp-9722) | 0.5159 | 0.000 | 4 |
Na2LiAlP2 (mp-9719) | 0.4995 | 0.000 | 4 |
K2LiInAs2 (mp-505431) | 0.4579 | 0.000 | 4 |
K3Na2SnBi3 (mp-568329) | 0.5274 | 0.000 | 4 |
K2NaInSb2 (mp-505767) | 0.5457 | 0.000 | 4 |
YbH2 (mp-864603) | 0.5027 | 0.000 | 2 |
CaH2 (mp-23713) | 0.5259 | 0.000 | 2 |
SrH2 (mp-23714) | 0.5201 | 0.000 | 2 |
SrAl2 (mp-1071777) | 0.5519 | 0.013 | 2 |
BaH2 (mp-23715) | 0.5077 | 0.000 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ta_pv Co P |
Final Energy/Atom-8.9501 eV |
Corrected Energy-107.4016 eV
Uncorrected energy = -107.4016 eV
Corrected energy = -107.4016 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)