Final Magnetic Moment-0.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingUnknown |
Formation Energy / Atom-0.636 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. |
Density8.07 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.022 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 MauguinPnma [62] |
Hall-P 2ac 2n |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 151.8 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 303.6 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 75.9 |
BaF2 (mp-1029) | <1 1 0> | <1 0 1> | 163.4 |
SiO2 (mp-6930) | <1 1 0> | <0 1 0> | 143.0 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 303.6 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 75.9 |
InAs (mp-20305) | <1 1 0> | <0 1 1> | 161.9 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 303.6 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 151.8 |
LiGaO2 (mp-5854) | <0 1 1> | <0 0 1> | 303.6 |
TeO2 (mp-2125) | <1 1 0> | <0 0 1> | 303.6 |
Fe3O4 (mp-19306) | <1 0 0> | <0 0 1> | 75.9 |
MgO (mp-1265) | <1 0 0> | <0 0 1> | 303.6 |
TiO2 (mp-2657) | <1 1 1> | <0 0 1> | 227.7 |
C (mp-66) | <1 1 0> | <0 1 1> | 161.9 |
Ge (mp-32) | <1 0 0> | <0 0 1> | 303.6 |
PbS (mp-21276) | <1 0 0> | <0 1 0> | 143.0 |
PbS (mp-21276) | <1 1 0> | <0 0 1> | 151.8 |
GaP (mp-2490) | <1 0 0> | <0 0 1> | 151.8 |
InP (mp-20351) | <1 0 0> | <0 1 0> | 143.0 |
InP (mp-20351) | <1 1 0> | <0 0 1> | 151.8 |
CaF2 (mp-2741) | <1 0 0> | <0 0 1> | 151.8 |
Fe2O3 (mp-24972) | <0 0 1> | <0 0 1> | 227.7 |
ZnTe (mp-2176) | <1 0 0> | <0 0 1> | 75.9 |
ZnTe (mp-2176) | <1 1 0> | <0 1 1> | 161.9 |
TbScO3 (mp-31119) | <1 1 0> | <0 0 1> | 303.6 |
Ni (mp-23) | <1 0 0> | <0 0 1> | 303.6 |
PbSe (mp-2201) | <1 0 0> | <0 0 1> | 75.9 |
PbSe (mp-2201) | <1 1 0> | <0 1 1> | 161.9 |
BaTiO3 (mp-5986) | <1 0 0> | <0 0 1> | 151.8 |
BaTiO3 (mp-5986) | <1 1 0> | <0 1 0> | 143.0 |
NdGaO3 (mp-3196) | <0 0 1> | <0 0 1> | 151.8 |
NdGaO3 (mp-3196) | <1 1 0> | <0 0 1> | 303.6 |
Ga2O3 (mp-886) | <1 0 0> | <0 0 1> | 303.6 |
Si (mp-149) | <1 0 0> | <0 0 1> | 151.8 |
CdSe (mp-2691) | <1 0 0> | <0 0 1> | 75.9 |
CdSe (mp-2691) | <1 1 0> | <0 1 1> | 161.9 |
C (mp-48) | <1 1 1> | <0 0 1> | 303.6 |
CaCO3 (mp-3953) | <1 1 0> | <0 0 1> | 151.8 |
Y3Fe5O12 (mp-19648) | <1 0 0> | <0 0 1> | 151.8 |
SiC (mp-8062) | <1 0 0> | <0 0 1> | 75.9 |
SiC (mp-8062) | <1 1 0> | <0 1 1> | 161.9 |
CsI (mp-614603) | <1 0 0> | <0 0 1> | 303.6 |
GaSb (mp-1156) | <1 0 0> | <0 0 1> | 75.9 |
GaSb (mp-1156) | <1 1 0> | <0 1 1> | 161.9 |
SrTiO3 (mp-4651) | <0 0 1> | <0 0 1> | 151.8 |
SrTiO3 (mp-4651) | <1 1 0> | <0 0 1> | 303.6 |
Cu (mp-30) | <1 1 1> | <0 0 1> | 227.7 |
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 |
---|---|---|---|
KTh(SbSe3)2 (mp-568904) | 0.6772 | 0.000 | 4 |
BaLa(BiS3)2 (mp-555699) | 0.6606 | 0.000 | 4 |
La5Sn4 (mp-30757) | 0.1284 | 0.000 | 2 |
Tb5Ge4 (mp-1673) | 0.1190 | 0.000 | 2 |
Y5Pb4 (mp-672188) | 0.1260 | 0.082 | 2 |
Sm5Ge4 (mp-1506) | 0.1378 | 0.000 | 2 |
Y5Ge4 (mp-13360) | 0.1305 | 0.000 | 2 |
Ce2Sc3Si4 (mp-505512) | 0.3320 | 0.000 | 3 |
Hf3(NbGe2)2 (mp-21659) | 0.4257 | 0.014 | 3 |
Hf4NbGe4 (mp-571038) | 0.4191 | 0.000 | 3 |
U2Nb3Ge4 (mp-21813) | 0.4576 | 0.000 | 3 |
Pr2Sc3Si4 (mp-568831) | 0.3927 | 0.000 | 3 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-points4 |
U Values-- |
PseudopotentialsVASP PAW: La Pb_d |
Final Energy/Atom-5.0171 eV |
Corrected Energy-180.6160 eV
-180.6160 eV = -180.6160 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)