Final Magnetic Moment0.000 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-0.339 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. |
Density5.53 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.487 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] |
---|---|---|---|
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 130.7 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 130.7 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 130.7 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 130.7 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 130.7 |
CdS (mp-672) | <1 1 1> | <0 0 1> | 261.5 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 261.5 |
BN (mp-984) | <1 0 1> | <0 0 1> | 261.5 |
BN (mp-984) | <1 1 1> | <0 1 1> | 169.5 |
Al (mp-134) | <1 0 0> | <0 0 1> | 130.7 |
GdScO3 (mp-5690) | <1 1 0> | <0 0 1> | 130.7 |
TbScO3 (mp-31119) | <1 1 0> | <0 0 1> | 130.7 |
ZnO (mp-2133) | <1 0 0> | <0 0 1> | 261.5 |
MgAl2O4 (mp-3536) | <1 0 0> | <0 0 1> | 130.7 |
Cu (mp-30) | <1 0 0> | <0 0 1> | 130.7 |
Ge (mp-32) | <1 0 0> | <0 0 1> | 130.7 |
LiAlO2 (mp-3427) | <1 0 1> | <0 0 1> | 130.7 |
GdScO3 (mp-5690) | <0 1 0> | <0 0 1> | 130.7 |
GdScO3 (mp-5690) | <1 1 1> | <0 1 0> | 215.9 |
Mg (mp-153) | <1 1 0> | <0 0 1> | 261.5 |
TbScO3 (mp-31119) | <0 1 0> | <0 0 1> | 130.7 |
C (mp-48) | <1 0 1> | <0 0 1> | 261.5 |
NaCl (mp-22862) | <1 0 0> | <0 0 1> | 130.7 |
ZrO2 (mp-2858) | <1 0 0> | <0 0 1> | 261.5 |
ZrO2 (mp-2858) | <1 0 1> | <0 0 1> | 130.7 |
SrTiO3 (mp-4651) | <1 1 1> | <0 1 0> | 215.9 |
LiAlO2 (mp-3427) | <1 1 1> | <0 0 1> | 261.5 |
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 |
---|---|---|---|
Bi2OF4 (mp-753309) | 0.6204 | 0.012 | 3 |
Nb3(CuTe3)2 (mp-675608) | 0.6175 | 0.277 | 3 |
Bi3O2F5 (mp-759405) | 0.6862 | 0.006 | 3 |
TaTe4I (mp-28691) | 0.5585 | 0.000 | 3 |
K3In2As3 (mp-583615) | 0.5967 | 0.000 | 3 |
Nb2Tl3CuSe12 (mp-570757) | 0.7001 | 0.000 | 4 |
MgSi2 (mp-1073493) | 0.6858 | 0.192 | 2 |
Mg6Si5 (mp-1073904) | 0.6800 | 0.183 | 2 |
Mg4Si3 (mp-1074264) | 0.6973 | 0.152 | 2 |
Mg3Si4 (mp-1075240) | 0.6987 | 0.216 | 2 |
MgSi2 (mp-1073387) | 0.7020 | 0.212 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Nb_pv Te I |
Final Energy/Atom-4.3718 eV |
Corrected Energy-226.3800 eV
Uncorrected energy = -209.8440 eV
Composition-based energy adjustment (-0.379 eV/atom x 8.0 atoms) = -3.0320 eV
Composition-based energy adjustment (-0.422 eV/atom x 32.0 atoms) = -13.5040 eV
Corrected energy = -226.3800 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)