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-3.438 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. |
Density2.91 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap5.416 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 MauguinP63/m [176] |
Hall-P 6c |
Point Group6/m |
Crystal Systemhexagonal |
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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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <1 0 0> | 251.6 |
AlN (mp-661) | <1 0 0> | <1 1 0> | 48.4 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 139.8 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 290.5 |
CeO2 (mp-20194) | <1 0 0> | <1 1 0> | 242.1 |
CeO2 (mp-20194) | <1 1 0> | <1 0 0> | 83.9 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 205.8 |
BaF2 (mp-1029) | <1 0 0> | <1 1 0> | 193.7 |
BaF2 (mp-1029) | <1 1 0> | <1 0 0> | 55.9 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 68.6 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 139.8 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 83.9 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 195.7 |
GaN (mp-804) | <1 1 0> | <1 0 0> | 335.4 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 335.4 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 195.7 |
SiO2 (mp-6930) | <1 0 0> | <1 1 0> | 290.5 |
SiO2 (mp-6930) | <1 1 0> | <1 0 1> | 148.1 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 205.8 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 55.9 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 68.6 |
LaAlO3 (mp-2920) | <1 1 0> | <1 0 0> | 251.6 |
LaAlO3 (mp-2920) | <1 1 1> | <1 0 0> | 251.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 0> | 223.6 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 1> | 296.3 |
DyScO3 (mp-31120) | <1 1 0> | <1 1 0> | 242.1 |
InAs (mp-20305) | <1 0 0> | <1 1 0> | 193.7 |
InAs (mp-20305) | <1 1 0> | <1 0 0> | 55.9 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 68.6 |
AlN (mp-661) | <0 0 1> | <1 0 0> | 83.9 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 363.4 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 363.4 |
CdS (mp-672) | <1 0 0> | <1 1 0> | 338.9 |
CdS (mp-672) | <1 0 1> | <1 0 1> | 296.3 |
LiF (mp-1138) | <1 0 0> | <1 1 0> | 338.9 |
LiF (mp-1138) | <1 1 0> | <1 0 0> | 223.6 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 205.8 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 111.8 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 274.4 |
Te2W (mp-22693) | <1 0 0> | <1 1 0> | 96.8 |
YVO4 (mp-19133) | <1 0 0> | <1 0 0> | 223.6 |
TePb (mp-19717) | <1 1 0> | <1 0 0> | 251.6 |
Te2Mo (mp-602) | <0 0 1> | <1 0 0> | 55.9 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 274.4 |
Ag (mp-124) | <1 0 0> | <1 0 1> | 296.3 |
BN (mp-984) | <1 1 0> | <0 0 1> | 68.6 |
LiNbO3 (mp-3731) | <0 0 1> | <1 0 0> | 139.8 |
LiNbO3 (mp-3731) | <1 1 0> | <1 0 0> | 251.6 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 0 0> | 223.6 |
MoS2 (mp-1434) | <0 0 1> | <1 0 0> | 139.8 |
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) |
||
---|---|---|
2.37 | 0.00 | 0.00 |
-0.00 | 2.37 | 0.00 |
0.00 | 0.00 | 2.29 |
Dielectric Tensor εij (total) |
||
---|---|---|
6.04 | 0.00 | 0.00 |
-0.00 | 6.04 | 0.00 |
0.00 | 0.00 | 5.84 |
Polycrystalline dielectric constant
εpoly∞
2.34
|
Polycrystalline dielectric constant
εpoly
5.98
|
Refractive Index n1.53 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
V5(BO5)2 (mp-772349) | 0.5232 | 0.034 | 3 |
Mg3(BO3)2 (mp-5005) | 0.5730 | 0.000 | 3 |
Co3(BO3)2 (mp-561056) | 0.5593 | 0.000 | 3 |
Ni3(BO3)2 (mp-18806) | 0.5626 | 0.000 | 3 |
Co3(BO3)2 (mp-24876) | 0.5440 | 0.000 | 3 |
Mg5B3O9F (mp-560026) | 0.5260 | 0.025 | 4 |
Li2V(CO3)2 (mp-765113) | 0.5163 | 0.141 | 4 |
LiCoCO4 (mp-763148) | 0.5844 | 0.076 | 4 |
Mg2BO3F (mp-7995) | 0.5411 | 0.000 | 4 |
LiVBO4 (mp-769715) | 0.4900 | 0.042 | 4 |
V8O15 (mp-565320) | 0.6079 | 0.156 | 2 |
V9O17 (mp-565758) | 0.6115 | 0.030 | 2 |
V6O11 (mp-510127) | 0.6376 | 0.013 | 2 |
V7O13 (mp-556332) | 0.6216 | 0.038 | 2 |
V7O13 (mp-623373) | 0.6265 | 0.038 | 2 |
RbLi2Cr2(BO3)3 (mp-770630) | 0.7255 | 0.216 | 5 |
Na3MgC2ClO6 (mp-23653) | 0.6859 | 0.000 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Mg_pv B O F |
Final Energy/Atom-6.2857 eV |
Corrected Energy-129.9275 eV
-129.9275 eV = -125.7138 eV (uncorrected energy) - 4.2137 eV (MP Anion Correction)
|
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)