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-1.053 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. |
Density4.60 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap3.912 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 MauguinPa3 [205] |
Hall-P 2ac 2ab 3 |
Point Groupm3 |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 213.9 |
CdS (mp-672) | <0 0 1> | <1 1 1> | 185.2 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 213.9 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 106.9 |
YVO4 (mp-19133) | <1 0 0> | <1 1 1> | 185.2 |
TePb (mp-19717) | <1 0 0> | <1 0 0> | 213.9 |
MoS2 (mp-1434) | <0 0 1> | <1 1 1> | 185.2 |
Al (mp-134) | <1 0 0> | <1 0 0> | 213.9 |
CdTe (mp-406) | <1 0 0> | <1 0 0> | 213.9 |
TiO2 (mp-2657) | <0 0 1> | <1 0 0> | 106.9 |
LaF3 (mp-905) | <0 0 1> | <1 1 1> | 185.2 |
PbS (mp-21276) | <1 1 0> | <1 1 0> | 151.2 |
PbS (mp-21276) | <1 1 1> | <1 1 1> | 185.2 |
InP (mp-20351) | <1 1 0> | <1 1 0> | 151.2 |
InP (mp-20351) | <1 1 1> | <1 1 1> | 185.2 |
InSb (mp-20012) | <1 0 0> | <1 0 0> | 213.9 |
WS2 (mp-224) | <0 0 1> | <1 1 1> | 185.2 |
Ge(Bi3O5)4 (mp-23352) | <1 1 0> | <1 1 0> | 151.2 |
YAlO3 (mp-3792) | <1 1 0> | <1 0 0> | 106.9 |
Ge(Bi3O5)4 (mp-23352) | <1 0 0> | <1 0 0> | 106.9 |
Ge(Bi3O5)4 (mp-23352) | <1 1 1> | <1 1 1> | 185.2 |
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 |
---|---|---|---|
Ca(BO2)2 (mp-13827) | 0.5176 | 0.041 | 3 |
Ba(MoN2)2 (mp-1029505) | 0.6240 | 0.004 | 3 |
Ba(VN2)2 (mp-1029918) | 0.4233 | 0.015 | 3 |
Ba(CrN2)2 (mp-1029568) | 0.3065 | 0.027 | 3 |
Sr(BO2)2 (mp-8878) | 0.2421 | 0.034 | 3 |
BaSr2(PN2)6 (mp-567486) | 0.3288 | 0.000 | 4 |
BaCa2(PN2)6 (mp-6404) | 0.5923 | 0.000 | 4 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv P N |
Final Energy/Atom-7.4178 eV |
Corrected Energy-623.0988 eV
-623.0988 eV = -623.0988 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)