Final Magnetic Moment3.414 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-3.387 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.473 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. |
Density5.00 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToBa4Bi3F17 + BaF2 + Bi |
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 MauguinR3m [160] |
HallR 3 2" |
Point Group3m |
Crystal Systemtrigonal |
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] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 217.2 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 217.2 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 217.2 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 334.2 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 200.5 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 300.8 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 217.2 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 150.4 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 50.1 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 334.2 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 217.2 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 200.5 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 66.8 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 117.0 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 350.9 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 250.6 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 200.5 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 66.8 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 284.0 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 334.2 |
SiO2 (mp-6930) | <1 1 1> | <0 0 1> | 267.3 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 200.5 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 66.8 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 250.6 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 267.3 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 267.3 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 66.8 |
ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 334.2 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 217.2 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 367.6 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 117.0 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 200.5 |
CdS (mp-672) | <1 1 1> | <0 0 1> | 317.5 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 117.0 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 267.3 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 217.2 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 150.4 |
Te2Mo (mp-602) | <1 0 0> | <0 0 1> | 267.3 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 350.9 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 350.9 |
TePb (mp-19717) | <1 1 0> | <0 0 1> | 250.6 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 267.3 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 117.0 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 16.7 |
Bi2Te3 (mp-34202) | <1 0 0> | <0 0 1> | 133.7 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 50.1 |
BN (mp-984) | <0 0 1> | <0 0 1> | 16.7 |
BN (mp-984) | <1 0 0> | <0 0 1> | 133.7 |
BN (mp-984) | <1 0 1> | <0 0 1> | 183.8 |
BN (mp-984) | <1 1 0> | <0 0 1> | 33.4 |
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 |
---|---|---|---|
Y2Th5O13 (mp-757205) | 0.5170 | 0.057 | 3 |
Ce5Sm2O13 (mp-753792) | 0.4963 | 0.036 | 3 |
Ce5Y2O13 (mp-753355) | 0.5350 | 0.043 | 3 |
Ce5Gd2O13 (mp-753088) | 0.5008 | 0.035 | 3 |
La2Th5O13 (mp-756142) | 0.4329 | 0.314 | 3 |
KLa2NbO6 (mp-554034) | 0.7219 | 0.000 | 4 |
KNd2NbO6 (mp-558128) | 0.7435 | 0.000 | 4 |
Zr27O49 (mp-684977) | 0.3884 | 0.116 | 2 |
U3O5 (mp-752998) | 0.3098 | 0.097 | 2 |
U12O19 (mp-684907) | 0.3328 | 0.138 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv Bi F |
Final Energy/Atom-5.1377 eV |
Corrected Energy-138.7183 eV
-138.7183 eV = -138.7183 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)