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-2.026 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.003 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. |
Density1.84 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLi2TeO3 |
Band Gap4.014 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 MauguinC2/m [12] |
Hall-C 2y |
Point Group2/m |
Crystal Systemmonoclinic |
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.
Apply Gaussian smoothing:
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> | <0 0 1> | 250.1 |
GaN (mp-804) | <0 0 1> | <1 1 1> | 161.2 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 50.0 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 200.1 |
CdS (mp-672) | <0 0 1> | <0 1 1> | 259.9 |
AlN (mp-661) | <1 0 0> | <0 1 0> | 141.4 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 200.1 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 264.0 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 -1> | 137.4 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 200.1 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 200.1 |
YVO4 (mp-19133) | <1 0 1> | <1 0 -1> | 137.4 |
YVO4 (mp-19133) | <1 1 0> | <0 0 1> | 200.1 |
BN (mp-984) | <1 0 0> | <0 0 1> | 250.1 |
LiNbO3 (mp-3731) | <0 0 1> | <0 1 1> | 259.9 |
LiNbO3 (mp-3731) | <1 0 0> | <0 0 1> | 150.1 |
LiNbO3 (mp-3731) | <1 0 1> | <0 0 1> | 150.1 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 1 1> | 259.9 |
MoS2 (mp-1434) | <1 0 0> | <0 0 1> | 200.1 |
Al (mp-134) | <1 1 0> | <1 0 -1> | 137.4 |
LiGaO2 (mp-5854) | <0 0 1> | <0 0 1> | 200.1 |
LiGaO2 (mp-5854) | <0 1 0> | <0 0 1> | 100.0 |
LiGaO2 (mp-5854) | <0 1 1> | <0 0 1> | 300.1 |
CdTe (mp-406) | <1 1 0> | <0 0 1> | 250.1 |
LiTaO3 (mp-3666) | <0 0 1> | <0 1 1> | 259.9 |
LiTaO3 (mp-3666) | <1 0 1> | <0 0 1> | 150.1 |
TiO2 (mp-2657) | <0 0 1> | <0 1 0> | 282.9 |
TiO2 (mp-2657) | <1 0 0> | <0 0 1> | 150.1 |
TiO2 (mp-2657) | <1 1 0> | <0 1 0> | 212.2 |
C (mp-66) | <1 0 0> | <0 1 0> | 141.4 |
C (mp-66) | <1 1 0> | <0 0 1> | 200.1 |
GdScO3 (mp-5690) | <0 1 1> | <1 0 0> | 264.0 |
Mg (mp-153) | <1 0 0> | <0 0 1> | 50.0 |
Mg (mp-153) | <1 1 0> | <0 0 1> | 200.1 |
GaP (mp-2490) | <1 1 0> | <1 0 0> | 132.0 |
TbScO3 (mp-31119) | <0 1 1> | <1 0 0> | 264.0 |
Ni (mp-23) | <1 0 0> | <0 1 0> | 282.9 |
Ni (mp-23) | <1 1 1> | <0 0 1> | 250.1 |
InSb (mp-20012) | <1 1 0> | <0 0 1> | 250.1 |
BaTiO3 (mp-5986) | <1 0 0> | <0 1 0> | 282.9 |
BaTiO3 (mp-5986) | <1 1 1> | <0 0 1> | 200.1 |
NdGaO3 (mp-3196) | <0 1 1> | <1 1 1> | 161.2 |
NdGaO3 (mp-3196) | <1 0 1> | <1 0 0> | 264.0 |
SiC (mp-11714) | <1 0 0> | <0 1 0> | 282.9 |
MoSe2 (mp-1634) | <0 0 1> | <0 1 0> | 212.2 |
WS2 (mp-224) | <1 0 0> | <1 0 -1> | 137.4 |
C (mp-48) | <0 0 1> | <0 1 0> | 212.2 |
C (mp-48) | <1 0 0> | <0 0 1> | 150.1 |
C (mp-48) | <1 0 1> | <0 1 1> | 259.9 |
WSe2 (mp-1821) | <0 0 1> | <0 1 0> | 212.2 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
CuP4I (mp-567472) | 0.7310 | 0.004 | 3 |
Cu3P15I2 (mp-679930) | 0.6476 | 0.000 | 3 |
Zn(SbO2)2 (mvc-6325) | 0.7400 | 0.224 | 3 |
Ga2TeSe2 (mp-28423) | 0.4979 | 0.000 | 3 |
Ga2TeS2 (mp-27255) | 0.4949 | 0.000 | 3 |
Cu3P4S4I3 (mp-565597) | 0.7396 | 0.000 | 4 |
In7Te10 (mp-669311) | 0.7332 | 0.000 | 2 |
Pb3N2 (mp-1080198) | 0.5082 | 0.338 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Li_sv Te O |
Final Energy/Atom-5.3093 eV |
Corrected Energy-67.9254 eV
-67.9254 eV = -63.7117 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)