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-0.986 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. |
Density3.38 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap1.409 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 1> | <1 0 0> | 272.4 |
AlN (mp-661) | <1 1 0> | <1 0 -1> | 331.9 |
BaF2 (mp-1029) | <1 1 0> | <1 1 -1> | 114.6 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 282.5 |
SiO2 (mp-6930) | <1 0 0> | <0 1 0> | 280.4 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 282.5 |
SiO2 (mp-6930) | <1 1 1> | <1 0 -1> | 265.5 |
LaAlO3 (mp-2920) | <0 0 1> | <1 0 -1> | 199.2 |
LaAlO3 (mp-2920) | <1 0 0> | <0 1 0> | 280.4 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 272.4 |
AlN (mp-661) | <1 1 1> | <1 0 -1> | 199.2 |
CeO2 (mp-20194) | <1 1 0> | <1 0 -1> | 331.9 |
GaN (mp-804) | <1 0 1> | <1 0 -1> | 132.8 |
GaN (mp-804) | <1 1 0> | <1 0 0> | 272.4 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 280.4 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 169.5 |
KCl (mp-23193) | <1 1 0> | <1 1 -1> | 114.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 0> | 272.4 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 -1> | 331.9 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 113.0 |
InAs (mp-20305) | <1 1 0> | <1 0 1> | 106.1 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 272.4 |
CdS (mp-672) | <0 0 1> | <1 1 -1> | 229.3 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 169.5 |
LiF (mp-1138) | <1 1 0> | <1 0 1> | 212.2 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 169.5 |
Te2Mo (mp-602) | <0 0 1> | <1 0 -1> | 66.4 |
Te2Mo (mp-602) | <1 0 0> | <1 0 -1> | 331.9 |
Te2Mo (mp-602) | <1 0 1> | <0 1 0> | 280.4 |
Te2Mo (mp-602) | <1 1 0> | <1 0 0> | 272.4 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 169.5 |
Ag (mp-124) | <1 1 0> | <1 0 0> | 272.4 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 -1> | 229.3 |
LiGaO2 (mp-5854) | <0 0 1> | <0 1 0> | 280.4 |
LiGaO2 (mp-5854) | <0 1 0> | <0 0 1> | 226.0 |
TeO2 (mp-2125) | <1 0 0> | <1 0 1> | 212.2 |
SiC (mp-7631) | <0 0 1> | <1 0 -1> | 66.4 |
SiC (mp-7631) | <1 0 1> | <0 0 1> | 282.5 |
Fe3O4 (mp-19306) | <1 0 0> | <0 0 1> | 226.0 |
TiO2 (mp-2657) | <1 0 0> | <0 0 1> | 56.5 |
TiO2 (mp-2657) | <1 0 1> | <1 0 -1> | 199.2 |
TiO2 (mp-2657) | <1 1 0> | <1 0 -1> | 199.2 |
GdScO3 (mp-5690) | <0 1 1> | <1 0 -1> | 331.9 |
Mg (mp-153) | <0 0 1> | <0 1 0> | 280.4 |
Mg (mp-153) | <1 1 1> | <0 0 1> | 282.5 |
LaF3 (mp-905) | <1 0 0> | <1 0 -1> | 331.9 |
Ga2O3 (mp-886) | <1 0 -1> | <0 0 1> | 113.0 |
Ga2O3 (mp-886) | <1 0 0> | <1 0 -1> | 265.5 |
Ga2O3 (mp-886) | <1 0 1> | <0 0 1> | 282.5 |
Si (mp-149) | <1 1 0> | <1 0 -1> | 331.9 |
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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Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
6.26 | 0.00 | 0.13 |
0.00 | 6.07 | 0.00 |
0.13 | 0.00 | 5.93 |
Dielectric Tensor εij (total) |
||
---|---|---|
17.24 | 0.00 | 1.74 |
0.00 | 15.41 | 0.00 |
1.74 | 0.00 | 18.27 |
Polycrystalline dielectric constant
εpoly∞
6.09
|
Polycrystalline dielectric constant
εpoly
16.97
|
Refractive Index n2.47 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Na4MnO4 (mp-853250) | 0.4813 | 0.000 | 3 |
K4PbO4 (mp-22328) | 0.5017 | 0.000 | 3 |
Sr4TiN4 (mp-1029799) | 0.4798 | 0.000 | 3 |
Ca4VN4 (mp-1029737) | 0.5146 | 0.042 | 3 |
Ca4SiN4 (mp-1019576) | 0.2789 | 0.000 | 3 |
Li6Co(SiO4)2 (mp-764961) | 0.5455 | 0.079 | 4 |
SnHg6(P2Cl3)2 (mp-568612) | 0.6907 | 0.000 | 4 |
Na4Mo(NO)2 (mp-18772) | 0.6324 | 0.062 | 4 |
Na4W(NO)2 (mp-19125) | 0.6514 | 0.157 | 4 |
Li6Fe(SiO4)2 (mp-768001) | 0.5464 | 0.071 | 4 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ca_sv Ge_d N |
Final Energy/Atom-5.9220 eV |
Corrected Energy-218.9666 eV
Uncorrected energy = -213.1906 eV
Composition-based energy adjustment (-0.361 eV/atom x 16.0 atoms) = -5.7760 eV
Corrected energy = -218.9666 eV
|
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)