Final Magnetic Moment0.024 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-2.677 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.092 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. |
Density2.15 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToYCl3 + BaCl2 |
Band Gap4.126 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 MauguinP21/c [14] |
Hall-P 2ybc |
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> | <0 0 1> | 139.9 |
CdS (mp-672) | <1 1 0> | <0 0 1> | 209.8 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 279.8 |
Te2Mo (mp-602) | <1 1 0> | <0 0 1> | 279.8 |
CdS (mp-672) | <1 1 1> | <0 0 1> | 209.8 |
BN (mp-984) | <0 0 1> | <0 0 1> | 279.8 |
SiC (mp-7631) | <1 0 0> | <0 0 1> | 139.9 |
LaF3 (mp-905) | <1 1 0> | <0 0 1> | 279.8 |
TiO2 (mp-2657) | <1 0 1> | <0 0 1> | 209.8 |
SiC (mp-11714) | <1 0 0> | <0 0 1> | 279.8 |
Mg (mp-153) | <1 0 1> | <0 0 1> | 279.8 |
LaF3 (mp-905) | <1 0 0> | <0 0 1> | 279.8 |
YAlO3 (mp-3792) | <0 1 0> | <0 0 1> | 279.8 |
YAlO3 (mp-3792) | <1 1 0> | <0 0 1> | 279.8 |
Ni (mp-23) | <1 0 0> | <0 0 1> | 279.8 |
CdWO4 (mp-19387) | <0 1 1> | <0 0 1> | 279.8 |
CdWO4 (mp-19387) | <1 1 1> | <0 0 1> | 209.8 |
NdGaO3 (mp-3196) | <0 1 1> | <0 0 1> | 209.8 |
NdGaO3 (mp-3196) | <1 0 1> | <0 0 1> | 209.8 |
Ga2O3 (mp-886) | <1 0 1> | <0 0 1> | 139.9 |
MgF2 (mp-1249) | <1 0 1> | <0 0 1> | 209.8 |
YAlO3 (mp-3792) | <1 0 0> | <0 0 1> | 279.8 |
LiAlO2 (mp-3427) | <1 1 0> | <0 0 1> | 139.9 |
LiAlO2 (mp-3427) | <1 1 1> | <0 0 1> | 279.8 |
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Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv Y_sv Cl |
Final Energy/Atom-5.0433 eV |
Corrected Energy-342.9446 eV
-342.9446 eV = -342.9446 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)