Final Magnetic Moment0.994 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-1.265 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.011 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. |
Density4.65 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLiNiO2 + Li(NiO2)2 |
Band Gap0.250 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/m [12] |
Hall-C 2y |
Point Group2/m |
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <1 0 0> | 160.8 |
LaAlO3 (mp-2920) | <1 0 0> | <1 0 0> | 225.1 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 160.8 |
AlN (mp-661) | <0 0 1> | <1 0 0> | 225.1 |
AlN (mp-661) | <1 0 0> | <1 1 0> | 173.7 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 128.6 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 56.4 |
AlN (mp-661) | <1 1 1> | <0 1 0> | 192.6 |
CeO2 (mp-20194) | <1 0 0> | <1 0 -1> | 93.0 |
CeO2 (mp-20194) | <1 1 0> | <1 0 0> | 128.6 |
GaAs (mp-2534) | <1 0 0> | <1 1 -1> | 66.9 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 48.1 |
GaAs (mp-2534) | <1 1 1> | <1 0 -1> | 232.6 |
GaN (mp-804) | <0 0 1> | <1 1 0> | 115.8 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 128.6 |
GaN (mp-804) | <1 1 1> | <1 0 1> | 237.3 |
SiO2 (mp-6930) | <0 0 1> | <1 1 0> | 173.7 |
SiO2 (mp-6930) | <1 1 0> | <1 0 0> | 96.5 |
KCl (mp-23193) | <1 0 0> | <1 0 -1> | 232.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 0> | 32.2 |
DyScO3 (mp-31120) | <0 1 0> | <1 1 -1> | 133.9 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 56.4 |
DyScO3 (mp-31120) | <1 1 1> | <1 1 1> | 277.8 |
ZnSe (mp-1190) | <1 1 1> | <1 0 -1> | 232.6 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 56.4 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 240.7 |
CdS (mp-672) | <1 1 1> | <1 1 -1> | 267.8 |
BaF2 (mp-1029) | <1 0 0> | <1 0 -1> | 232.6 |
Te2W (mp-22693) | <0 1 1> | <1 0 1> | 237.3 |
GaN (mp-804) | <1 0 0> | <1 1 1> | 185.2 |
GaN (mp-804) | <1 1 0> | <1 0 -1> | 232.6 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 56.4 |
SiO2 (mp-6930) | <1 0 1> | <1 1 1> | 277.8 |
YVO4 (mp-19133) | <1 0 1> | <1 1 1> | 277.8 |
YVO4 (mp-19133) | <1 1 1> | <0 0 1> | 169.1 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 225.1 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 0> | 225.1 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 -1> | 186.1 |
Te2Mo (mp-602) | <0 0 1> | <1 0 -1> | 279.1 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 0> | 257.3 |
InAs (mp-20305) | <1 0 0> | <1 0 -1> | 232.6 |
ZnSe (mp-1190) | <1 0 0> | <1 1 -1> | 66.9 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 48.1 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 32.2 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 112.7 |
CdS (mp-672) | <1 0 0> | <1 0 -1> | 232.6 |
LiF (mp-1138) | <1 0 0> | <1 1 -1> | 66.9 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 48.1 |
LiF (mp-1138) | <1 1 1> | <1 1 0> | 57.9 |
BN (mp-984) | <1 0 0> | <1 0 0> | 353.8 |
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 |
---|---|---|---|
Li3(NiO2)4 (mp-764850) | 0.1896 | 0.062 | 3 |
Li3(CoO2)4 (mp-764781) | 0.1891 | 0.121 | 3 |
Li4(NiO2)5 (mp-763578) | 0.2028 | 0.048 | 3 |
Li3(NiO2)4 (mp-850106) | 0.1259 | 0.015 | 3 |
Li3(NiO2)4 (mvc-16810) | 0.1796 | 0.017 | 3 |
Li3MnNi3O8 (mp-762583) | 0.1587 | 0.202 | 4 |
Li3Co2(NiO4)2 (mp-779959) | 0.1682 | 0.017 | 4 |
Li3Mn2(NiO4)2 (mp-763752) | 0.1349 | 0.495 | 4 |
Li3Mn2(CoO4)2 (mp-778583) | 0.1629 | 0.415 | 4 |
Li3Ti2(NiO4)2 (mp-763633) | 0.1695 | 0.074 | 4 |
Fe8O9 (mp-763787) | 0.3173 | 0.063 | 2 |
Fe9O10 (mp-763441) | 0.2895 | 0.350 | 2 |
Fe7O8 (mp-715333) | 0.2387 | 0.064 | 2 |
Fe8O9 (mp-705588) | 0.2459 | 0.050 | 2 |
Fe10O11 (mp-705555) | 0.3068 | 0.046 | 2 |
Li6Mn3Cr2Fe3O16 (mp-861553) | 0.4199 | 0.882 | 5 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesNi: 6.2 eV |
PseudopotentialsVASP PAW: Li_sv Ni_pv O |
Final Energy/Atom-4.8758 eV |
Corrected Energy-87.4112 eV
-87.4112 eV = -73.1369 eV (uncorrected energy) - 8.6560 eV (MP Advanced Correction) - 5.6183 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)