Final Magnetic Moment4.000 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-1.208 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.149 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. |
Density4.79 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLi2CoNi3O8 + Li(CoO2)2 |
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 MauguinImma [74] |
Hall-I 2b 2 |
Point Groupmmm |
Crystal Systemorthorhombic |
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) | <0 0 1> | <0 1 1> | 336.9 |
AlN (mp-661) | <1 0 0> | <1 1 1> | 217.5 |
AlN (mp-661) | <1 1 0> | <1 1 1> | 217.5 |
AlN (mp-661) | <1 1 1> | <1 1 1> | 145.0 |
CeO2 (mp-20194) | <1 0 0> | <1 1 0> | 259.2 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 32.5 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 45.8 |
GaAs (mp-2534) | <1 1 1> | <0 1 0> | 228.8 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 162.7 |
AlN (mp-661) | <0 0 1> | <0 1 0> | 228.8 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 194.4 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 260.3 |
GaN (mp-804) | <1 0 1> | <0 1 0> | 228.8 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 162.7 |
GaN (mp-804) | <1 1 0> | <0 1 0> | 91.5 |
GaN (mp-804) | <1 1 1> | <0 1 0> | 320.3 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 137.3 |
KCl (mp-23193) | <1 1 0> | <0 1 0> | 183.0 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 91.5 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 45.8 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 292.8 |
SiO2 (mp-6930) | <0 0 1> | <1 0 1> | 168.8 |
SiO2 (mp-6930) | <1 0 0> | <1 1 1> | 217.5 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 162.7 |
DyScO3 (mp-31120) | <0 1 0> | <1 1 0> | 129.6 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 1> | 217.5 |
DyScO3 (mp-31120) | <1 0 1> | <0 1 1> | 56.1 |
DyScO3 (mp-31120) | <1 1 0> | <1 1 0> | 64.8 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 45.8 |
ZnSe (mp-1190) | <1 1 1> | <0 1 0> | 228.8 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 0> | 45.8 |
KTaO3 (mp-3614) | <1 1 1> | <0 1 1> | 56.1 |
CdS (mp-672) | <1 1 0> | <0 1 1> | 336.9 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 32.5 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 324.0 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 32.5 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 32.5 |
CdS (mp-672) | <0 0 1> | <1 1 0> | 324.0 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 45.8 |
LiF (mp-1138) | <1 1 1> | <0 1 1> | 56.1 |
Te2W (mp-22693) | <0 1 1> | <0 0 1> | 292.8 |
YVO4 (mp-19133) | <1 0 0> | <1 1 1> | 145.0 |
YVO4 (mp-19133) | <1 0 1> | <0 1 1> | 280.7 |
CdS (mp-672) | <1 0 0> | <0 1 0> | 320.3 |
CdS (mp-672) | <1 0 1> | <0 1 0> | 228.8 |
CdS (mp-672) | <1 1 1> | <1 1 0> | 259.2 |
YVO4 (mp-19133) | <0 0 1> | <1 1 0> | 259.2 |
TePb (mp-19717) | <1 1 0> | <0 1 0> | 183.0 |
Te2Mo (mp-602) | <0 0 1> | <0 1 1> | 336.9 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 162.7 |
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 |
---|---|---|---|
Al2CdSe4 (mp-3807) | 0.0461 | 0.047 | 3 |
MgAl2O4 (mp-3536) | 0.0404 | 0.000 | 3 |
LiMn2O4 (mp-25015) | 0.0466 | 0.047 | 3 |
MnCr2O4 (mp-541022) | 0.0429 | 0.000 | 3 |
CaIn2O4 (mp-22766) | 0.0416 | 0.000 | 3 |
Li2Cr3FeO8 (mp-774415) | 0.0769 | 0.605 | 4 |
Li2CoNi3O8 (mp-761777) | 0.0492 | 0.016 | 4 |
Li2MnCo3O8 (mp-761737) | 0.0720 | 0.028 | 4 |
Li2Co3NiO8 (mp-761738) | 0.0368 | 0.221 | 4 |
Li2MnFe3O8 (mp-775094) | 0.0356 | 0.095 | 4 |
Co3O4 (mp-559191) | 0.1119 | 0.046 | 2 |
In3S4 (mp-556597) | 0.2005 | 0.042 | 2 |
Co3O4 (mp-18748) | 0.0409 | 0.046 | 2 |
Sn3N4 (mp-16031) | 0.2218 | 0.000 | 2 |
Ge3N4 (mp-476) | 0.2573 | 0.109 | 2 |
Li4Cr2Fe3Co3O16 (mp-775698) | 0.4277 | 0.897 | 5 |
Li4Mn2Fe3Co3O16 (mp-761441) | 0.4352 | 0.078 | 5 |
Li14Mn22Cr3Cu3O56 (mp-735790) | 0.3999 | 0.014 | 5 |
Li4Mn3Cr3(CuO8)2 (mp-765456) | 0.4066 | 0.069 | 5 |
Li4Cr3Cu3(SbO8)2 (mp-783908) | 0.4331 | 0.035 | 5 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesCo: 3.32 eVNi: 6.2 eV |
PseudopotentialsVASP PAW: Li_sv Co Ni_pv O |
Final Energy/Atom-5.1709 eV |
Corrected Energy-86.2469 eV
Uncorrected energy = -72.3929 eV
Composition-based energy adjustment (-0.687 eV/atom x 8.0 atoms) = -5.4960 eV
Composition-based energy adjustment (-1.638 eV/atom x 2.0 atoms) = -3.2760 eV
Composition-based energy adjustment (-2.541 eV/atom x 2.0 atoms) = -5.0820 eV
Corrected energy = -86.2469 eV
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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)