Final Magnetic Moment-0.768 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFerri |
Formation Energy / Atom0.251 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.355 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. |
Density7.31 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToEuZn5 + Zn |
Band Gap0.014 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 MauguinFm3c [226] |
Hall-F 4c 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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
Apply Gaussian smoothing:
Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
KCd13 (mp-397) | 0.1543 | 0.000 | 2 |
RbCd13 (mp-1040) | 0.1511 | 0.000 | 2 |
CsCd13 (mp-1713) | 0.1450 | 0.000 | 2 |
BaZn13 (mp-672225) | 0.1826 | 0.000 | 2 |
SrZn13 (mp-672707) | 0.1835 | 0.000 | 2 |
LaCoCu12 (mp-13486) | 0.3405 | 0.000 | 3 |
BaSi4Cu9 (mp-11143) | 0.4993 | 0.000 | 3 |
SrCu9Ge4 (mp-11144) | 0.2775 | 0.000 | 3 |
BaCu9Ge4 (mp-11145) | 0.2944 | 0.000 | 3 |
LaFe9Si4 (mp-662529) | 0.4317 | 0.013 | 3 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-points14 |
U Values-- |
PseudopotentialsVASP PAW: Eu Zn |
Final Energy/Atom-1.6669 eV |
Corrected Energy-46.6732 eV
-46.6732 eV = -46.6732 eV (uncorrected energy)
|
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)