Final Magnetic Moment0.022 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-0.343 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. |
Density4.35 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.803 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] |
---|---|---|---|
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 120.3 |
GaN (mp-804) | <1 1 0> | <1 0 0> | 264.1 |
Te2W (mp-22693) | <0 1 0> | <1 0 0> | 264.1 |
BN (mp-984) | <1 0 1> | <0 0 1> | 120.3 |
BN (mp-984) | <1 1 0> | <1 0 0> | 132.1 |
SiC (mp-7631) | <1 0 1> | <0 0 1> | 240.5 |
SiC (mp-7631) | <1 0 0> | <0 0 1> | 240.5 |
TiO2 (mp-2657) | <1 0 0> | <1 0 1> | 179.3 |
GaP (mp-2490) | <1 0 0> | <0 0 1> | 120.3 |
NdGaO3 (mp-3196) | <1 1 0> | <0 0 1> | 120.3 |
NdGaO3 (mp-3196) | <1 1 1> | <1 0 0> | 132.1 |
MoSe2 (mp-1634) | <1 0 0> | <1 0 0> | 264.1 |
MoSe2 (mp-1634) | <1 1 0> | <1 0 0> | 264.1 |
NdGaO3 (mp-3196) | <1 0 0> | <1 0 0> | 132.1 |
WSe2 (mp-1821) | <1 1 0> | <1 0 0> | 264.1 |
Si (mp-149) | <1 0 0> | <0 0 1> | 120.3 |
C (mp-48) | <1 1 0> | <1 0 0> | 132.1 |
ZrO2 (mp-2858) | <1 1 1> | <1 0 0> | 264.1 |
CaCO3 (mp-3953) | <1 0 0> | <1 0 0> | 264.1 |
CsI (mp-614603) | <1 0 0> | <0 0 1> | 120.3 |
CsI (mp-614603) | <1 1 0> | <1 0 0> | 264.1 |
SrTiO3 (mp-4651) | <1 1 0> | <0 0 1> | 120.3 |
SrTiO3 (mp-4651) | <1 0 0> | <1 0 0> | 132.1 |
CaF2 (mp-2741) | <1 0 0> | <0 0 1> | 120.3 |
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 |
---|---|---|---|
Na2Al2Sb3 (mp-30039) | 0.3182 | 0.000 | 3 |
Rb2In2Sb3 (mp-21760) | 0.1936 | 0.000 | 3 |
K2Al2Sb3 (mp-17886) | 0.3141 | 0.000 | 3 |
Na2Ga2As3 (mp-15431) | 0.3384 | 0.000 | 3 |
K2Ga2Sb3 (mp-15433) | 0.3161 | 0.000 | 3 |
SrLi4NiO4 (mp-778288) | 0.6758 | 0.263 | 4 |
BaLi4NiO4 (mp-776790) | 0.6574 | 0.105 | 4 |
K3Na2InO4 (mp-553975) | 0.6879 | 0.000 | 4 |
LiCaGaN2 (mp-570948) | 0.6322 | 0.000 | 4 |
LiCaAlN2 (mp-1020031) | 0.5916 | 0.000 | 4 |
MgSi2 (mp-1073470) | 0.6598 | 0.211 | 2 |
MgSi2 (mp-1073528) | 0.5502 | 0.150 | 2 |
Mg5Si9 (mp-1075658) | 0.6634 | 0.198 | 2 |
Mg5Si9 (mp-1075724) | 0.6631 | 0.253 | 2 |
CdO2 (mp-1096876) | 0.6658 | 0.515 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: K_sv In_d Sb |
Final Energy/Atom-3.2164 eV |
Corrected Energy-184.7244 eV
Uncorrected energy = -180.1164 eV
Composition-based energy adjustment (-0.192 eV/atom x 24.0 atoms) = -4.6080 eV
Corrected energy = -184.7244 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)