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-3.279 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. |
Density6.37 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap4.553 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 MauguinPnma [62] |
Hall-P 2ac 2n |
Point Groupmmm |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 200.6 |
LaAlO3 (mp-2920) | <1 0 0> | <0 1 1> | 213.5 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 302.1 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 164.2 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 127.7 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 71.7 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 54.7 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 54.7 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 145.9 |
CeO2 (mp-20194) | <1 1 0> | <1 0 0> | 120.8 |
GaAs (mp-2534) | <1 0 0> | <0 1 0> | 193.0 |
GaAs (mp-2534) | <1 1 0> | <1 0 0> | 181.3 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 193.0 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 164.2 |
LiF (mp-1138) | <1 1 1> | <0 1 0> | 115.8 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 237.1 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 286.8 |
Te2W (mp-22693) | <0 0 1> | <0 1 1> | 42.7 |
Te2W (mp-22693) | <0 1 0> | <0 1 0> | 154.4 |
Te2W (mp-22693) | <0 1 1> | <0 1 0> | 115.8 |
Te2W (mp-22693) | <1 0 0> | <1 1 0> | 286.8 |
GaN (mp-804) | <0 0 1> | <1 1 0> | 71.7 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 120.8 |
GaN (mp-804) | <1 0 1> | <0 1 1> | 170.8 |
GaN (mp-804) | <1 1 0> | <1 0 0> | 60.4 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 145.9 |
YVO4 (mp-19133) | <1 0 0> | <1 0 1> | 189.4 |
YVO4 (mp-19133) | <1 0 1> | <0 0 1> | 273.6 |
YVO4 (mp-19133) | <1 1 0> | <0 0 1> | 127.7 |
YVO4 (mp-19133) | <1 1 1> | <0 0 1> | 164.2 |
SiO2 (mp-6930) | <0 0 1> | <0 1 0> | 347.5 |
SiO2 (mp-6930) | <1 0 0> | <0 1 0> | 115.8 |
SiO2 (mp-6930) | <1 0 1> | <0 1 1> | 170.8 |
SiO2 (mp-6930) | <1 1 0> | <0 1 0> | 193.0 |
SiO2 (mp-6930) | <1 1 1> | <1 0 1> | 315.6 |
KCl (mp-23193) | <1 0 0> | <1 1 0> | 286.8 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 286.8 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 218.9 |
Te2Mo (mp-602) | <1 1 0> | <1 1 0> | 286.8 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 200.6 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 273.6 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 346.5 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 0> | 60.4 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 1> | 126.2 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 255.4 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 181.3 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 0> | 215.1 |
DyScO3 (mp-31120) | <1 1 1> | <0 0 1> | 273.6 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 310.1 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 310.1 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Na2Mn2O3 (mp-566788) | 0.4205 | 0.000 | 3 |
LiDyO2 (mp-976726) | 0.0379 | 0.000 | 3 |
LiEuO2 (mp-1019724) | 0.1191 | 1.034 | 3 |
Na2Mn2O3 (mp-607868) | 0.4241 | 0.000 | 3 |
LiGdO2 (mp-21332) | 0.0583 | 0.000 | 3 |
Li3V4SnO12 (mp-775037) | 0.4975 | 0.069 | 4 |
Li2Co4OF8 (mp-765686) | 0.4986 | 0.643 | 4 |
Li3Nb4NiO12 (mp-772009) | 0.4711 | 0.089 | 4 |
Li4Fe2OF8 (mp-776724) | 0.4987 | 0.036 | 4 |
LiCoOF2 (mp-849507) | 0.4869 | 0.345 | 4 |
Fe2O3 (mp-715276) | 0.4924 | 0.086 | 2 |
Al2O3 (mp-776490) | 0.5102 | 0.048 | 2 |
Fe2O3 (mp-542309) | 0.5178 | 0.131 | 2 |
Al2O3 (mp-1938) | 0.4778 | 0.093 | 2 |
Ca3N2 (mp-568293) | 0.5221 | 0.032 | 2 |
Li4Fe3Co2Sn3O16 (mp-775387) | 0.7088 | 0.260 | 5 |
Li4V2Cr3Fe3O16 (mp-770523) | 0.6828 | 0.264 | 5 |
Li4V2Co3Cu3O16 (mp-763156) | 0.7133 | 0.088 | 5 |
Li4V2Co3Ni3O16 (mp-763125) | 0.6991 | 0.119 | 5 |
Li4MnV2WO12 (mp-773239) | 0.6676 | 0.088 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Li_sv Tb_3 O |
Final Energy/Atom-7.0380 eV |
Corrected Energy-118.1040 eV
Uncorrected energy = -112.6080 eV
Composition-based energy adjustment (-0.687 eV/atom x 8.0 atoms) = -5.4960 eV
Corrected energy = -118.1040 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)