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-1.129 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. |
Density4.35 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.585 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 MauguinPbam [55] |
Hall-P 2 2ab |
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <0 0 1> | 135.8 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 142.9 |
LaAlO3 (mp-2920) | <1 0 0> | <0 1 0> | 142.9 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 158.9 |
LiGaO2 (mp-5854) | <1 0 0> | <0 1 0> | 142.9 |
TeO2 (mp-2125) | <0 1 0> | <0 0 1> | 135.8 |
KP(HO2)2 (mp-23959) | <1 1 0> | <0 1 0> | 142.9 |
Ni (mp-23) | <1 0 0> | <1 0 0> | 158.9 |
BaTiO3 (mp-5986) | <1 1 0> | <0 1 0> | 142.9 |
ZrO2 (mp-2858) | <0 1 0> | <0 1 1> | 197.1 |
YAlO3 (mp-3792) | <1 0 1> | <0 1 1> | 197.1 |
Y3Fe5O12 (mp-19648) | <1 0 0> | <1 0 0> | 158.9 |
SiC (mp-8062) | <1 1 1> | <0 0 1> | 135.8 |
ZnO (mp-2133) | <1 0 1> | <1 0 0> | 158.9 |
Cu (mp-30) | <1 0 0> | <0 1 1> | 197.1 |
GaTe (mp-542812) | <1 0 0> | <0 0 1> | 135.8 |
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 |
---|---|---|---|
Yb15Mg5Ge16 (mp-686293) | 0.7191 | 0.073 | 3 |
K5(Mo6S7)4 (mp-676371) | 0.7422 | 0.265 | 3 |
Li2Mo3S4 (mp-675779) | 0.6894 | 0.000 | 3 |
Bi9AuBr9 (mp-684015) | 0.6900 | 0.052 | 3 |
Ba4P3 (mp-28823) | 0.4399 | 0.000 | 2 |
MgSi2 (mp-1073530) | 0.7302 | 0.235 | 2 |
MgSi2 (mp-1073539) | 0.7204 | 0.183 | 2 |
Mg5Si6 (mp-1075403) | 0.7410 | 0.201 | 2 |
Ag7Te4 (mp-28228) | 0.7281 | 0.233 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Sr_sv As |
Final Energy/Atom-4.0907 eV |
Corrected Energy-229.0792 eV
-229.0792 eV = -229.0792 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)