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-3.848 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. |
Density6.16 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap3.499 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 MauguinC2221 [20] |
HallC 2c 2 |
Point Group222 |
Crystal Systemorthorhombic |
Topological Classificationtrivial*
|
SubclassificationLCEBR†
|
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 1 0> | <1 0 0> | 237.8 |
AlN (mp-661) | <0 0 1> | <1 0 0> | 237.8 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 195.3 |
AlN (mp-661) | <1 1 1> | <1 0 1> | 113.1 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 241.9 |
CeO2 (mp-20194) | <1 1 0> | <0 1 0> | 171.0 |
GaAs (mp-2534) | <1 0 0> | <0 1 0> | 285.1 |
BaF2 (mp-1029) | <1 1 0> | <1 0 0> | 158.5 |
BaF2 (mp-1029) | <1 1 1> | <1 1 0> | 195.3 |
GaN (mp-804) | <1 0 0> | <0 1 0> | 171.0 |
GaN (mp-804) | <1 1 0> | <1 0 0> | 237.8 |
SiO2 (mp-6930) | <0 0 1> | <1 1 0> | 195.3 |
SiO2 (mp-6930) | <1 0 1> | <1 0 0> | 317.0 |
SiO2 (mp-6930) | <1 1 0> | <0 1 0> | 285.1 |
SiO2 (mp-6930) | <1 1 1> | <1 0 0> | 158.5 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 237.8 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 285.1 |
InAs (mp-20305) | <1 1 0> | <1 0 0> | 158.5 |
InAs (mp-20305) | <1 1 1> | <1 1 0> | 195.3 |
ZnSe (mp-1190) | <1 0 0> | <0 1 0> | 285.1 |
KTaO3 (mp-3614) | <1 1 1> | <1 1 0> | 195.3 |
CdS (mp-672) | <1 0 1> | <0 1 0> | 342.1 |
CdS (mp-672) | <1 1 1> | <1 1 1> | 253.2 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 285.1 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 285.1 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 161.3 |
TePb (mp-19717) | <1 1 0> | <1 0 0> | 237.8 |
Te2Mo (mp-602) | <1 0 0> | <1 0 0> | 158.5 |
Ag (mp-124) | <1 0 0> | <1 0 1> | 226.1 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 1 0> | 171.0 |
BN (mp-984) | <0 0 1> | <0 1 1> | 98.7 |
BN (mp-984) | <1 0 0> | <0 1 0> | 57.0 |
BN (mp-984) | <1 1 0> | <1 1 0> | 97.6 |
BN (mp-984) | <1 1 1> | <0 1 0> | 228.1 |
LiNbO3 (mp-3731) | <0 0 1> | <0 1 0> | 285.1 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 0> | 195.3 |
Al (mp-134) | <1 1 1> | <1 1 0> | 195.3 |
LiGaO2 (mp-5854) | <1 0 0> | <1 0 0> | 317.0 |
LiGaO2 (mp-5854) | <1 1 0> | <1 1 0> | 97.6 |
CdTe (mp-406) | <1 0 0> | <1 0 1> | 226.1 |
CdTe (mp-406) | <1 1 0> | <1 0 0> | 237.8 |
SiC (mp-7631) | <1 0 1> | <0 1 0> | 228.1 |
LiTaO3 (mp-3666) | <0 0 1> | <0 1 0> | 285.1 |
Fe3O4 (mp-19306) | <1 0 0> | <0 1 0> | 285.1 |
MgO (mp-1265) | <1 0 0> | <0 1 0> | 285.1 |
TiO2 (mp-2657) | <0 0 1> | <0 1 0> | 285.1 |
TiO2 (mp-2657) | <1 0 0> | <1 0 0> | 317.0 |
Ge3(BiO3)4 (mp-23560) | <1 1 1> | <1 1 0> | 195.3 |
C (mp-66) | <1 1 0> | <0 0 1> | 161.3 |
GdScO3 (mp-5690) | <0 0 1> | <0 1 0> | 285.1 |
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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Piezoelectric Tensor eij (C/m2) |
|||||
---|---|---|---|---|---|
0.00000 | 0.00000 | 0.00000 | -0.08390 | 0.00000 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | 0.00000 | 0.01511 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | 0.00000 | 0.00000 | -0.34066 |
Piezoelectric Modulus ‖eij‖max0.34066 C/m2 |
Crystallographic Direction vmax |
---|
0.00000 |
-1.00000 |
0.00000 |
Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
4.58 | 0.00 | 0.00 |
0.00 | 4.60 | 0.00 |
0.00 | 0.00 | 4.42 |
Dielectric Tensor εij (total) |
||
---|---|---|
22.72 | 0.00 | 0.00 |
0.00 | 23.97 | 0.00 |
0.00 | 0.00 | 24.83 |
Polycrystalline dielectric constant
εpoly∞
4.53
|
Polycrystalline dielectric constant
εpoly
23.84
|
Refractive Index n2.13 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Tm3TaO7 (mp-769931) | 0.2726 | 0.011 | 3 |
Ho3TaO7 (mp-31416) | 0.0619 | 0.000 | 3 |
Sm3NbO7 (mp-756591) | 0.2763 | 0.002 | 3 |
Er3TaO7 (mp-755898) | 0.2792 | 0.006 | 3 |
Ho3ReO7 (mp-558969) | 0.1520 | 0.045 | 3 |
Na2InCuF7 (mp-21611) | 0.4898 | 0.009 | 4 |
Ca2Zr5Ti2O16 (mp-667369) | 0.6767 | 0.000 | 4 |
Na2ScCuF7 (mp-21527) | 0.5199 | 0.025 | 4 |
Na2InNiF7 (mp-557278) | 0.6046 | 0.000 | 4 |
Na2MgInF7 (mp-10837) | 0.5751 | 0.000 | 4 |
Bi4O7 (mp-30303) | 0.5436 | 0.000 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Y_sv Ta_pv O |
Final Energy/Atom-9.3917 eV |
Corrected Energy-216.2347 eV
Uncorrected energy = -206.6167 eV
Composition-based energy adjustment (-0.687 eV/atom x 14.0 atoms) = -9.6180 eV
Corrected energy = -216.2347 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)