Final Magnetic Moment1.553 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-1.674 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.115 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. |
Density4.69 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLiCoO2 + CoO |
Band Gap0.045 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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 0 0> | <1 0 1> | 218.5 |
AlN (mp-661) | <1 0 1> | <0 1 0> | 266.9 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 310.4 |
GaAs (mp-2534) | <1 0 0> | <1 0 -1> | 230.9 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 112.7 |
GaN (mp-804) | <1 1 1> | <1 -1 -1> | 298.7 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 310.4 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 112.7 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 186.3 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 112.7 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 -1> | 230.9 |
CdS (mp-672) | <1 0 0> | <1 0 -1> | 230.9 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 266.9 |
Te2W (mp-22693) | <0 1 0> | <1 0 -1> | 154.0 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 186.3 |
Ag (mp-124) | <1 1 0> | <0 1 0> | 266.9 |
BN (mp-984) | <1 0 0> | <0 0 1> | 310.4 |
BN (mp-984) | <1 0 1> | <1 0 -1> | 307.9 |
BN (mp-984) | <1 1 0> | <1 -1 0> | 239.1 |
BN (mp-984) | <1 1 1> | <0 0 1> | 248.4 |
MoS2 (mp-1434) | <1 0 0> | <1 -1 1> | 204.9 |
Al (mp-134) | <1 0 0> | <1 0 -1> | 230.9 |
Al (mp-134) | <1 1 0> | <1 0 -1> | 230.9 |
LiGaO2 (mp-5854) | <0 0 1> | <0 0 1> | 310.4 |
LiGaO2 (mp-5854) | <0 1 0> | <1 0 0> | 284.9 |
LiGaO2 (mp-5854) | <1 0 1> | <1 0 -1> | 307.9 |
LiGaO2 (mp-5854) | <1 1 0> | <1 -1 0> | 239.1 |
LiGaO2 (mp-5854) | <1 1 1> | <1 0 0> | 284.9 |
SiC (mp-7631) | <0 0 1> | <0 0 1> | 310.4 |
SiC (mp-7631) | <1 0 0> | <1 -1 0> | 239.1 |
TiO2 (mp-2657) | <1 1 0> | <0 1 -1> | 299.3 |
C (mp-66) | <1 1 0> | <0 1 0> | 200.2 |
Mg (mp-153) | <1 1 1> | <1 -1 -1> | 298.7 |
LaF3 (mp-905) | <1 1 1> | <1 1 -1> | 104.1 |
PbS (mp-21276) | <1 1 0> | <0 0 1> | 248.4 |
GaP (mp-2490) | <1 1 0> | <0 0 1> | 310.4 |
InP (mp-20351) | <1 1 0> | <0 0 1> | 248.4 |
TbScO3 (mp-31119) | <0 0 1> | <1 0 0> | 284.9 |
TbScO3 (mp-31119) | <1 0 0> | <0 0 1> | 186.3 |
Ni (mp-23) | <1 0 0> | <0 1 0> | 133.4 |
Ni (mp-23) | <1 1 1> | <1 0 0> | 213.7 |
PbSe (mp-2201) | <1 1 0> | <1 1 0> | 112.7 |
BaTiO3 (mp-5986) | <1 0 0> | <0 0 1> | 310.4 |
BaTiO3 (mp-5986) | <1 0 1> | <0 0 1> | 186.3 |
BaTiO3 (mp-5986) | <1 1 1> | <1 0 -1> | 230.9 |
NdGaO3 (mp-3196) | <0 1 0> | <0 0 1> | 310.4 |
SiC (mp-11714) | <0 0 1> | <0 0 1> | 310.4 |
SiC (mp-11714) | <1 0 1> | <1 1 0> | 225.4 |
MoSe2 (mp-1634) | <0 0 1> | <0 0 1> | 310.4 |
MoSe2 (mp-1634) | <1 0 0> | <0 0 1> | 248.4 |
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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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Li4Ni7O11 (mp-768091) | 0.1301 | 0.031 | 3 |
Li7Ni9O16 (mp-768059) | 0.1473 | 0.021 | 3 |
Li19Ni23O42 (mp-698842) | 0.1392 | 0.000 | 3 |
Li5Mn7O12 (mp-773337) | 0.1396 | 0.042 | 3 |
LiNiO2 (mp-850062) | 0.1430 | 0.009 | 3 |
Li5Mn5Cr2O12 (mp-771509) | 0.1348 | 0.042 | 4 |
Li10FeNi9O20 (mp-769545) | 0.1380 | 0.004 | 4 |
Li5Co2Ni5O12 (mp-766767) | 0.1341 | 0.042 | 4 |
Li5Fe2Co5O12 (mp-766146) | 0.1405 | 0.096 | 4 |
Li3Co(NiO2)4 (mp-771785) | 0.1261 | 0.020 | 4 |
Te2Au (mp-1662) | 0.3590 | 0.018 | 2 |
NaTe3 (mp-28478) | 0.4115 | 0.000 | 2 |
LiTe3 (mp-27466) | 0.2868 | 0.009 | 2 |
Sb2Te3 (mp-1080789) | 0.4203 | 0.129 | 2 |
Te2Au (mp-567525) | 0.3894 | 0.018 | 2 |
Na6MnNi3(SbO6)2 (mp-1094109) | 0.4514 | 0.005 | 5 |
Hg (mp-982872) | 0.6131 | 0.020 | 1 |
Sb (mp-632286) | 0.5140 | 0.059 | 1 |
Te (mp-570459) | 0.5181 | 0.044 | 1 |
Te (mp-10654) | 0.6590 | 0.047 | 1 |
Te (mp-105) | 0.5265 | 0.047 | 1 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesCo: 3.32 eV |
PseudopotentialsVASP PAW: Li_sv Co O |
Final Energy/Atom-5.6421 eV |
Corrected Energy-363.7324 eV
-363.7324 eV = -315.9583 eV (uncorrected energy) - 28.1100 eV (MP Advanced Correction) - 19.6641 eV (MP Anion Correction)
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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)