Final Magnetic Moment29.003 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-1.775 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.130 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. |
Density4.63 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToFe2O3 + LiFeO2 + LiCoO2 |
Band Gap0.587 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 [5] |
HallC 2y |
Point Group2 |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <0 0 1> | 226.5 |
AlN (mp-661) | <1 0 1> | <0 1 1> | 266.4 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 135.9 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 244.1 |
GaN (mp-804) | <1 0 1> | <0 1 1> | 133.2 |
GaN (mp-804) | <1 1 0> | <0 1 0> | 341.7 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 317.1 |
SiO2 (mp-6930) | <0 0 1> | <0 1 0> | 195.3 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 135.9 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 317.1 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 176.4 |
KCl (mp-23193) | <1 1 1> | <1 0 -1> | 274.0 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 264.5 |
DyScO3 (mp-31120) | <1 0 1> | <0 1 0> | 292.9 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 1> | 212.7 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 226.5 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 226.5 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 135.9 |
ZnSe (mp-1190) | <1 0 0> | <0 1 0> | 341.7 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 317.1 |
CdS (mp-672) | <1 0 0> | <0 1 0> | 341.7 |
CdS (mp-672) | <1 0 1> | <1 1 1> | 234.1 |
CdS (mp-672) | <1 1 0> | <0 1 1> | 199.8 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 341.7 |
LiF (mp-1138) | <1 1 0> | <0 1 1> | 266.4 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 90.6 |
Te2W (mp-22693) | <0 0 1> | <0 1 0> | 244.1 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 271.8 |
Te2Mo (mp-602) | <1 0 0> | <0 0 1> | 271.8 |
Te2Mo (mp-602) | <1 0 1> | <0 1 1> | 333.0 |
Ag (mp-124) | <1 0 0> | <0 1 0> | 244.1 |
Ag (mp-124) | <1 1 0> | <0 1 1> | 266.4 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 90.6 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 135.9 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 90.6 |
BN (mp-984) | <0 0 1> | <0 0 1> | 226.5 |
BN (mp-984) | <1 0 0> | <0 0 1> | 317.1 |
BN (mp-984) | <1 0 1> | <0 0 1> | 317.1 |
BN (mp-984) | <1 1 0> | <0 0 1> | 135.9 |
BN (mp-984) | <1 1 1> | <1 0 -1> | 274.0 |
LiNbO3 (mp-3731) | <1 1 1> | <1 0 0> | 264.5 |
AlN (mp-661) | <0 0 1> | <0 1 0> | 341.7 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 135.9 |
AlN (mp-661) | <1 1 1> | <0 1 0> | 341.7 |
Al (mp-134) | <1 0 0> | <0 0 1> | 317.1 |
Al (mp-134) | <1 1 1> | <0 1 0> | 146.5 |
GaAs (mp-2534) | <1 0 0> | <0 1 0> | 341.7 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 317.1 |
BaF2 (mp-1029) | <1 1 0> | <0 0 1> | 226.5 |
LiGaO2 (mp-5854) | <0 0 1> | <0 0 1> | 135.9 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Li3Fe7O12 (mp-762465) | 0.1132 | 0.107 | 3 |
Li5Fe5O12 (mp-762602) | 0.2219 | 0.695 | 3 |
Li3V7O12 (mp-762285) | 0.1647 | 0.078 | 3 |
Li5V5O12 (mp-762939) | 0.2126 | 0.156 | 3 |
Li3Fe2Ni5O12 (mp-997540) | 0.1710 | 0.077 | 4 |
Li3Cr2Fe5O12 (mp-780009) | 0.1737 | 0.967 | 4 |
Li3Mn5Cr2O12 (mp-850947) | 0.1624 | 0.084 | 4 |
Li3Mn2Ni5O12 (mp-762611) | 0.1602 | 0.061 | 4 |
Li3V5Cr2O12 (mp-781743) | 0.1340 | 0.079 | 4 |
Ni6O7 (mp-767815) | 0.2780 | 0.047 | 2 |
Ni5O6 (mp-782702) | 0.3002 | 0.041 | 2 |
V6C5 (mp-28731) | 0.2500 | 0.000 | 2 |
Fe7O8 (mp-715333) | 0.3191 | 0.064 | 2 |
Ni6Cl7 (mp-1022720) | 0.2324 | 0.376 | 2 |
Li6Mn3Cr2Fe3O16 (mp-861553) | 0.4191 | 0.882 | 5 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesFe: 5.3 eVCo: 3.32 eV |
PseudopotentialsVASP PAW: Li_sv Fe_pv Co O |
Final Energy/Atom-6.1312 eV |
Corrected Energy-160.7260 eV
-160.7260 eV = -134.8855 eV (uncorrected energy) - 17.4130 eV (MP Advanced Correction) - 8.4275 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)