Final Magnetic Moment0.103 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-2.562 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. |
Density5.76 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
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 MauguinC2/m [12] |
Hall-C 2y |
Point Group2/m |
Crystal Systemmonoclinic |
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] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <1 0 -1> | 204.4 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 -1> | 204.4 |
BN (mp-984) | <1 1 0> | <1 0 0> | 172.0 |
BN (mp-984) | <1 1 1> | <0 0 1> | 234.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 0> | 258.1 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 1> | 178.6 |
Al (mp-134) | <1 0 0> | <1 0 1> | 178.6 |
Al (mp-134) | <1 1 0> | <1 0 -1> | 204.4 |
CdTe (mp-406) | <1 1 0> | <1 0 0> | 258.1 |
TeO2 (mp-2125) | <0 0 1> | <1 0 0> | 258.1 |
MgO (mp-1265) | <1 1 0> | <1 0 0> | 258.1 |
GdScO3 (mp-5690) | <0 0 1> | <1 0 0> | 258.1 |
InSb (mp-20012) | <1 1 0> | <1 0 0> | 258.1 |
BaTiO3 (mp-5986) | <1 0 1> | <0 0 1> | 117.3 |
GdScO3 (mp-5690) | <1 0 0> | <0 0 1> | 234.6 |
TbScO3 (mp-31119) | <0 0 1> | <1 0 0> | 258.1 |
BaTiO3 (mp-5986) | <0 0 1> | <1 0 0> | 258.1 |
BaTiO3 (mp-5986) | <1 0 0> | <1 0 -1> | 102.2 |
NdGaO3 (mp-3196) | <1 1 1> | <1 0 -1> | 204.4 |
Ga2O3 (mp-886) | <1 0 0> | <1 0 0> | 258.1 |
C (mp-48) | <1 0 0> | <1 0 0> | 172.0 |
C (mp-48) | <1 0 1> | <1 0 0> | 258.1 |
C (mp-48) | <1 1 0> | <1 0 0> | 172.0 |
SrTiO3 (mp-4651) | <1 1 1> | <1 0 -1> | 204.4 |
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 |
---|---|---|---|
La(ErS2)3 (mp-973441) | 0.6679 | 0.000 | 3 |
Yb11(U2S11)2 (mp-683986) | 0.6838 | 0.230 | 3 |
Gd(LuS2)3 (mp-22563) | 0.6760 | 0.000 | 3 |
Sm(ErS2)3 (mp-13283) | 0.6779 | 0.000 | 3 |
Ce(YS2)3 (mp-1006324) | 0.6812 | 0.000 | 3 |
In3Bi7(Pb2S9)2 (mp-651005) | 0.7227 | 0.032 | 4 |
Er2S3 (mp-9092) | 0.7471 | 0.009 | 2 |
Tm2S3 (mp-2309) | 0.7441 | 0.026 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: La Er_3 S |
Final Energy/Atom-6.5669 eV |
Corrected Energy-315.6580 eV
Uncorrected energy = -302.0770 eV
Composition-based energy adjustment (-0.503 eV/atom x 27.0 atoms) = -13.5810 eV
Corrected energy = -315.6580 eV
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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)