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-1.560 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.078 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. |
Density5.20 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToBaZrSe3 |
Band Gap0.261 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 MauguinP1 [1] |
HallP 1 |
Point Group1 |
Crystal Systemtriclinic |
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> | 196.0 |
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 140.0 |
LaAlO3 (mp-2920) | <1 1 0> | <0 1 1> | 118.8 |
AlN (mp-661) | <1 1 1> | <0 1 1> | 277.3 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 364.1 |
BaF2 (mp-1029) | <1 1 0> | <0 1 1> | 158.5 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 84.0 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 252.0 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 84.0 |
GaN (mp-804) | <1 0 1> | <1 1 1> | 242.7 |
GaN (mp-804) | <1 1 0> | <0 1 1> | 118.8 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 252.0 |
AlN (mp-661) | <1 0 1> | <1 1 1> | 194.2 |
AlN (mp-661) | <1 1 0> | <0 1 1> | 79.2 |
CeO2 (mp-20194) | <1 0 0> | <1 1 0> | 119.2 |
CeO2 (mp-20194) | <1 1 0> | <0 1 0> | 84.2 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 140.0 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 194.2 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 84.0 |
GaN (mp-804) | <0 0 1> | <1 1 1> | 145.6 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 194.2 |
SiO2 (mp-6930) | <1 0 0> | <1 1 1> | 339.8 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 252.7 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 336.0 |
SiO2 (mp-6930) | <1 1 1> | <0 1 1> | 158.5 |
InAs (mp-20305) | <1 1 0> | <0 1 1> | 158.5 |
InAs (mp-20305) | <1 1 1> | <1 1 1> | 194.2 |
KCl (mp-23193) | <1 0 0> | <1 1 1> | 242.7 |
KCl (mp-23193) | <1 1 0> | <0 1 1> | 118.8 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 1> | 119.0 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 1> | 158.6 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 252.0 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 140.0 |
CdS (mp-672) | <1 0 1> | <0 1 1> | 198.1 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 364.1 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 140.0 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 140.0 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 194.2 |
Te2W (mp-22693) | <0 0 1> | <0 1 1> | 237.7 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 1> | 356.5 |
KTaO3 (mp-3614) | <1 1 1> | <1 1 1> | 194.2 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 140.0 |
CdS (mp-672) | <1 1 0> | <0 1 1> | 158.5 |
TePb (mp-19717) | <1 1 0> | <0 1 1> | 118.8 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 224.0 |
Te2Mo (mp-602) | <1 0 0> | <0 1 1> | 158.5 |
Te2Mo (mp-602) | <1 0 1> | <0 1 1> | 277.3 |
Te2W (mp-22693) | <0 1 0> | <0 1 1> | 158.5 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 252.0 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 224.0 |
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 |
---|---|---|---|
TlCdF3 (mp-998623) | 0.2711 | 0.009 | 3 |
CaTlF3 (mp-998150) | 0.2702 | 0.018 | 3 |
CsSrI3 (mp-998417) | 0.2509 | 0.032 | 3 |
TlGeBr3 (mp-998153) | 0.2746 | 0.028 | 3 |
CaTlF3 (mp-1097061) | 0.2744 | 0.018 | 3 |
SrTaNO2 (mp-754505) | 0.2726 | 0.013 | 4 |
Ba2VFeO6 (mp-1096782) | 0.3319 | 0.101 | 4 |
Ba2LuIrO6 (mp-562274) | 0.3347 | 0.000 | 4 |
Sr2FeWO6 (mp-555520) | 0.3388 | 0.204 | 4 |
Sr2CrOsO6 (mp-1078448) | 0.3377 | 0.000 | 4 |
Mn4N (mp-637576) | 0.4618 | 1.987 | 2 |
Fe2O3 (mp-1068212) | 0.4594 | 0.860 | 2 |
Fe4P (mp-20885) | 0.4679 | 0.695 | 2 |
Ni4O (mp-1094082) | 0.4683 | 1.616 | 2 |
Ni4N (mp-1094090) | 0.4683 | 0.067 | 2 |
K2Ba6Yb3Bi5O24 (mp-684786) | 0.3050 | 0.014 | 5 |
Ba4Ta2TiZnO12 (mp-676665) | 0.2764 | 0.009 | 5 |
Ba6Sr2CoCu7O24 (mp-1076247) | 0.2859 | 0.080 | 5 |
Ba3SrCo(CuO4)3 (mp-1099886) | 0.2952 | 0.093 | 5 |
La7SmNi6(AgO12)2 (mp-1076723) | 0.2826 | 0.131 | 5 |
Na5Ca2Ce3Ti8Nb2O30 (mp-721094) | 0.6399 | 0.065 | 6 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv Zr_sv Se |
Final Energy/Atom-5.7506 eV |
Corrected Energy-28.7532 eV
-28.7532 eV = -28.7532 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)