Final Magnetic Moment0.005 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-1.963 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.011 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. |
Density5.58 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToBi2S3 + La2S3 |
Band Gap1.077 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] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 210.3 |
GaAs (mp-2534) | <1 0 0> | <0 1 0> | 231.3 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 231.3 |
GaN (mp-804) | <1 0 0> | <0 1 1> | 254.1 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 157.7 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 315.4 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 231.3 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 315.4 |
ZnSe (mp-1190) | <1 0 0> | <0 1 0> | 231.3 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 231.3 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 210.3 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 0> | 115.7 |
CdS (mp-672) | <1 0 0> | <0 1 1> | 254.1 |
CdS (mp-672) | <1 0 1> | <0 1 0> | 231.3 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 115.7 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 210.3 |
YVO4 (mp-19133) | <1 1 0> | <0 0 1> | 262.8 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 262.8 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 262.8 |
BN (mp-984) | <0 0 1> | <0 0 1> | 262.8 |
Al (mp-134) | <1 0 0> | <0 0 1> | 210.3 |
Al (mp-134) | <1 1 0> | <0 1 0> | 115.7 |
LiGaO2 (mp-5854) | <0 1 0> | <0 0 1> | 262.8 |
LiGaO2 (mp-5854) | <1 0 1> | <0 0 1> | 315.4 |
CdTe (mp-406) | <1 0 0> | <0 0 1> | 262.8 |
TeO2 (mp-2125) | <1 1 1> | <0 0 1> | 105.1 |
TiO2 (mp-2657) | <0 0 1> | <0 0 1> | 262.8 |
TiO2 (mp-2657) | <1 0 0> | <0 0 1> | 262.8 |
TiO2 (mp-2657) | <1 1 0> | <0 0 1> | 157.7 |
C (mp-66) | <1 0 0> | <0 0 1> | 315.4 |
C (mp-66) | <1 1 0> | <0 0 1> | 315.4 |
GdScO3 (mp-5690) | <0 1 0> | <0 0 1> | 315.4 |
GdScO3 (mp-5690) | <1 0 0> | <0 1 0> | 231.3 |
GdScO3 (mp-5690) | <1 1 0> | <0 0 1> | 315.4 |
Ga2O3 (mp-886) | <1 0 0> | <0 0 1> | 315.4 |
Ga2O3 (mp-886) | <1 1 1> | <0 0 1> | 262.8 |
Au (mp-81) | <1 1 0> | <0 0 1> | 315.4 |
C (mp-48) | <1 0 0> | <0 0 1> | 210.3 |
C (mp-48) | <1 1 1> | <0 1 0> | 231.3 |
NaCl (mp-22862) | <1 0 0> | <0 1 0> | 231.3 |
NaCl (mp-22862) | <1 1 0> | <0 1 0> | 231.3 |
TbScO3 (mp-31119) | <0 1 0> | <0 0 1> | 315.4 |
TbScO3 (mp-31119) | <1 0 0> | <0 1 0> | 231.3 |
TbScO3 (mp-31119) | <1 1 0> | <0 0 1> | 315.4 |
InSb (mp-20012) | <1 0 0> | <0 0 1> | 262.8 |
ZrO2 (mp-2858) | <1 0 0> | <0 0 1> | 315.4 |
ZrO2 (mp-2858) | <1 0 1> | <0 0 1> | 210.3 |
BaTiO3 (mp-5986) | <0 0 1> | <0 1 1> | 127.1 |
BaTiO3 (mp-5986) | <1 0 0> | <0 1 1> | 254.1 |
BaTiO3 (mp-5986) | <1 0 1> | <0 1 0> | 115.7 |
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 |
---|---|---|---|
La3LuSe6 (mp-645695) | 0.6096 | 0.000 | 3 |
Er3CrS6 (mp-18420) | 0.5820 | 0.003 | 3 |
Tb3CrSe6 (mp-505638) | 0.5957 | 0.000 | 3 |
Sm3CrSe6 (mp-10386) | 0.6028 | 0.002 | 3 |
Sc(US2)3 (mp-21583) | 0.6128 | 0.025 | 3 |
KSm2Sb3Se8 (mp-567322) | 0.5999 | 0.005 | 4 |
AgBi2S3Cl (mp-558368) | 0.7399 | 0.008 | 4 |
Tb8CrTe13Cl (mp-570277) | 0.6943 | 0.067 | 4 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: La Bi S |
Final Energy/Atom-5.8816 eV |
Corrected Energy-376.7790 eV
-376.7790 eV = -352.8944 eV (uncorrected energy) - 23.8846 eV (MP Anion Correction)
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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)