Final Magnetic Moment0.339 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFiM |
Formation Energy / Atom-0.916 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.545 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. |
Density6.09 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLiCoO2 + CoO |
Band Gap0.000 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 MauguinP1 [2] |
Hall-P 1 |
Point Group1 |
Crystal Systemtriclinic |
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> | <1 0 1> | 219.6 |
AlN (mp-661) | <1 0 1> | <0 1 1> | 126.4 |
AlN (mp-661) | <1 1 0> | <1 0 -1> | 303.9 |
AlN (mp-661) | <1 1 1> | <1 -1 0> | 316.0 |
CeO2 (mp-20194) | <1 1 0> | <1 0 0> | 216.2 |
GaAs (mp-2534) | <1 1 0> | <1 0 0> | 270.2 |
LaAlO3 (mp-2920) | <1 0 0> | <1 0 0> | 216.2 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 216.2 |
BaF2 (mp-1029) | <1 1 1> | <0 1 0> | 141.7 |
AlN (mp-661) | <0 0 1> | <1 0 1> | 219.6 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 200.2 |
SiO2 (mp-6930) | <1 0 0> | <1 -1 0> | 252.8 |
GaAs (mp-2534) | <1 0 0> | <1 0 -1> | 303.9 |
BaF2 (mp-1029) | <1 1 0> | <0 1 0> | 283.4 |
GaN (mp-804) | <1 0 1> | <0 1 1> | 252.8 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 238.3 |
GaN (mp-804) | <1 1 1> | <0 1 0> | 236.1 |
SiO2 (mp-6930) | <0 0 1> | <0 1 0> | 283.4 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 280.3 |
KCl (mp-23193) | <1 1 0> | <0 1 0> | 236.1 |
KCl (mp-23193) | <1 1 1> | <0 1 0> | 141.7 |
DyScO3 (mp-31120) | <0 0 1> | <1 -1 -1> | 280.7 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 324.3 |
InAs (mp-20305) | <1 0 0> | <0 1 0> | 188.9 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 160.2 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 162.1 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 283.4 |
CdS (mp-672) | <1 0 1> | <1 1 0> | 158.9 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 280.3 |
TePb (mp-19717) | <1 1 0> | <0 1 0> | 236.1 |
Te2Mo (mp-602) | <0 0 1> | <0 1 0> | 330.6 |
Te2Mo (mp-602) | <1 0 1> | <1 1 -1> | 166.4 |
Te2Mo (mp-602) | <1 1 0> | <0 1 1> | 189.6 |
Ag (mp-124) | <1 0 0> | <1 0 -1> | 303.9 |
Ag (mp-124) | <1 1 0> | <0 1 1> | 126.4 |
BN (mp-984) | <0 0 1> | <0 1 0> | 141.7 |
BN (mp-984) | <1 0 0> | <0 1 0> | 236.1 |
BN (mp-984) | <1 0 1> | <1 0 0> | 216.2 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 216.2 |
DyScO3 (mp-31120) | <1 0 0> | <1 1 0> | 238.3 |
DyScO3 (mp-31120) | <1 1 1> | <1 1 1> | 283.1 |
LiNbO3 (mp-3731) | <0 0 1> | <1 -1 0> | 189.6 |
LiNbO3 (mp-3731) | <1 0 1> | <1 -1 0> | 316.0 |
ZnSe (mp-1190) | <1 0 0> | <1 0 -1> | 303.9 |
ZnSe (mp-1190) | <1 1 0> | <1 0 0> | 270.2 |
ZnSe (mp-1190) | <1 1 1> | <0 1 0> | 330.6 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 200.2 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 320.3 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 200.2 |
CdS (mp-672) | <1 1 0> | <0 0 1> | 200.2 |
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 |
---|---|---|---|
LiNi9O10 (mp-775737) | 0.0700 | 0.024 | 3 |
LiCo8O9 (mp-772385) | 0.0784 | 0.094 | 3 |
CaMn7O8 (mp-767029) | 0.0826 | 0.033 | 3 |
MnNi3O4 (mp-763867) | 0.0815 | 0.064 | 3 |
Li3Co13O16 (mp-767934) | 0.0715 | 0.493 | 3 |
HfMg14MnO16 (mp-1099135) | 0.0763 | 0.184 | 4 |
LiMg30WO32 (mp-1098411) | 0.0764 | 0.023 | 4 |
LiMg30WO32 (mp-1040082) | 0.0719 | 0.023 | 4 |
KC (mp-1064300) | 0.1757 | 2.337 | 2 |
KN (mp-1064647) | 0.1812 | 1.464 | 2 |
KC (mp-1064814) | 0.1545 | 2.337 | 2 |
CsI (mp-1078801) | 0.1777 | 0.003 | 2 |
MnO (mp-714882) | 0.1859 | 0.000 | 2 |
Hg (mp-982872) | 0.2170 | 0.020 | 1 |
Se (mp-7755) | 0.2170 | 0.181 | 1 |
K (mp-998881) | 0.2338 | 0.120 | 1 |
Te (mp-10654) | 0.2092 | 0.047 | 1 |
P (mp-53) | 0.2294 | 0.144 | 1 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesCo: 3.32 eV |
PseudopotentialsVASP PAW: Li_sv Co O |
Final Energy/Atom-5.5521 eV |
Corrected Energy-217.0152 eV
-217.0152 eV = -177.6686 eV (uncorrected energy) - 28.1100 eV (MP Advanced Correction) - 11.2366 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)