Final Magnetic Moment0.002 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-1.754 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.014 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 ToSrI2 + BaI2 |
Band Gap3.432 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 MauguinP4b2 [117] |
HallP 4 2ab |
Point Group42m |
Crystal Systemtetragonal |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
GaN (mp-804) | <1 0 1> | <0 0 1> | 206.5 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 275.4 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 68.8 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 68.8 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 275.4 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 275.4 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 275.4 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 68.8 |
Al (mp-134) | <1 0 0> | <0 0 1> | 275.4 |
LiGaO2 (mp-5854) | <1 0 1> | <0 0 1> | 137.7 |
LiGaO2 (mp-5854) | <0 1 1> | <0 0 1> | 206.5 |
Fe3O4 (mp-19306) | <1 0 0> | <0 0 1> | 68.8 |
PbS (mp-21276) | <1 0 0> | <0 0 1> | 68.8 |
TiO2 (mp-2657) | <0 0 1> | <0 0 1> | 275.4 |
Mg (mp-153) | <1 0 1> | <0 0 1> | 206.5 |
BaTiO3 (mp-5986) | <0 0 1> | <0 0 1> | 275.4 |
Mg (mp-153) | <1 1 1> | <0 0 1> | 275.4 |
GaP (mp-2490) | <1 0 0> | <0 0 1> | 275.4 |
NdGaO3 (mp-3196) | <0 0 1> | <0 0 1> | 275.4 |
InP (mp-20351) | <1 0 0> | <0 0 1> | 68.8 |
Si (mp-149) | <1 0 0> | <0 0 1> | 275.4 |
Au (mp-81) | <1 0 0> | <0 0 1> | 68.8 |
NaCl (mp-22862) | <1 1 0> | <0 0 1> | 137.7 |
ZrO2 (mp-2858) | <0 0 1> | <0 0 1> | 137.7 |
ZrO2 (mp-2858) | <1 1 0> | <0 0 1> | 275.4 |
MgAl2O4 (mp-3536) | <1 0 0> | <0 0 1> | 68.8 |
YAlO3 (mp-3792) | <1 1 0> | <0 0 1> | 275.4 |
ZnO (mp-2133) | <1 1 1> | <0 0 1> | 275.4 |
CaF2 (mp-2741) | <1 0 0> | <0 0 1> | 275.4 |
SrTiO3 (mp-4651) | <0 0 1> | <0 0 1> | 275.4 |
Ge (mp-32) | <1 0 0> | <0 0 1> | 68.8 |
LiAlO2 (mp-3427) | <0 0 1> | <0 0 1> | 137.7 |
LiAlO2 (mp-3427) | <1 1 1> | <0 0 1> | 275.4 |
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 |
---|---|---|---|
MgU2O6 (mp-686040) | 0.2113 | 0.029 | 3 |
MgCoF4 (mvc-14233) | 0.1955 | 0.117 | 3 |
TiZnF4 (mvc-3135) | 0.2362 | 0.346 | 3 |
Li5SnP3 (mp-675621) | 0.2295 | 0.013 | 3 |
BaSr2I6 (mp-772861) | 0.2101 | 0.033 | 3 |
PbF2 (mp-685150) | 0.3066 | 0.003 | 2 |
Mg2Ni (mp-1077177) | 0.3051 | 0.218 | 2 |
CeSe2 (mp-1080251) | 0.3133 | 0.011 | 2 |
CeSe2 (mp-1080346) | 0.3072 | 0.011 | 2 |
CeSe2 (mp-1080348) | 0.2691 | 0.014 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv Sr_sv I |
Final Energy/Atom-3.3846 eV |
Corrected Energy-121.8441 eV
-121.8441 eV = -121.8441 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)