Final Magnetic Moment2.000 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-1.167 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.062 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. |
Density4.40 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLiNiO2 + Li(NiO2)2 |
Band Gap0.390 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 MauguinAea2 [41] |
HallA 2 2ac |
Point Groupmm2 |
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <0 1 1> | 330.1 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 128.0 |
AlN (mp-661) | <1 0 1> | <0 1 0> | 251.9 |
AlN (mp-661) | <1 1 0> | <0 1 1> | 132.0 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 298.6 |
GaN (mp-804) | <1 1 0> | <1 0 1> | 289.7 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 213.3 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 42.7 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 213.3 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 213.3 |
SiO2 (mp-6930) | <1 1 1> | <0 0 1> | 213.3 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 251.9 |
DyScO3 (mp-31120) | <0 1 1> | <0 1 1> | 264.1 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 1> | 330.1 |
LaAlO3 (mp-2920) | <0 0 1> | <0 1 1> | 330.1 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 170.7 |
InAs (mp-20305) | <1 0 0> | <0 1 0> | 201.5 |
ZnSe (mp-1190) | <1 0 0> | <0 1 0> | 251.9 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 85.3 |
GaAs (mp-2534) | <1 0 0> | <0 1 0> | 251.9 |
BaF2 (mp-1029) | <1 0 0> | <0 1 0> | 201.5 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 251.9 |
CdS (mp-672) | <1 0 1> | <1 0 0> | 259.9 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 341.3 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 341.3 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 85.3 |
SiO2 (mp-6930) | <1 1 0> | <1 0 1> | 96.6 |
KCl (mp-23193) | <1 0 0> | <0 1 0> | 201.5 |
DyScO3 (mp-31120) | <1 1 0> | <0 1 0> | 251.9 |
DyScO3 (mp-31120) | <1 1 1> | <0 0 1> | 298.6 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 213.3 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 128.0 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 256.0 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 341.3 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 341.3 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 151.1 |
CdS (mp-672) | <1 0 0> | <1 0 1> | 289.7 |
CdS (mp-672) | <1 1 0> | <0 0 1> | 298.6 |
YVO4 (mp-19133) | <1 0 0> | <0 0 1> | 341.3 |
YVO4 (mp-19133) | <1 1 0> | <0 1 0> | 251.9 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 341.3 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 213.3 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 298.6 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 85.3 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 298.6 |
GaSe (mp-1943) | <0 0 1> | <0 1 1> | 264.1 |
BN (mp-984) | <0 0 1> | <0 1 1> | 66.0 |
BN (mp-984) | <1 0 0> | <0 1 0> | 151.1 |
BN (mp-984) | <1 0 1> | <0 0 1> | 256.0 |
BN (mp-984) | <1 1 0> | <1 0 0> | 259.9 |
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.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Li2Cr3O6 (mp-771534) | 0.3004 | 0.098 | 3 |
Li5Fe5O12 (mp-771687) | 0.2305 | 0.095 | 3 |
Li2Mn3O6 (mp-773276) | 0.3135 | 0.098 | 3 |
TlIn5Se7 (mp-574279) | 0.5511 | 0.020 | 3 |
TlIn5S7 (mp-562480) | 0.5074 | 0.000 | 3 |
Li4FeNi5O12 (mp-771577) | 0.1630 | 0.074 | 4 |
Li4Mn5CoO12 (mp-771545) | 0.1710 | 0.086 | 4 |
Li4Fe5NiO12 (mp-770801) | 0.1443 | 0.106 | 4 |
Li4MnNi5O12 (mp-779228) | 0.1912 | 0.066 | 4 |
Li4Fe5CoO12 (mp-769792) | 0.1905 | 0.107 | 4 |
Tl4O3 (mp-27684) | 0.7163 | 0.000 | 2 |
In6Se7 (mp-567596) | 0.5610 | 0.042 | 2 |
In6S7 (mp-555853) | 0.5092 | 0.008 | 2 |
Li4Ti4MnCr4O18 (mp-769442) | 0.5841 | 0.092 | 5 |
Li4Ti4V4CoO18 (mp-769478) | 0.6086 | 0.092 | 5 |
Li4Ti4Mn(Fe2O9)2 (mp-769443) | 0.6025 | 0.087 | 5 |
Li4Ti2V3Cr4O18 (mp-775447) | 0.6179 | 0.084 | 5 |
Li4Ti4VCr4O18 (mp-775391) | 0.6169 | 0.085 | 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-4.8157 eV |
Corrected Energy-127.3567 eV
-127.3567 eV = -105.9452 eV (uncorrected energy) - 12.9840 eV (MP Advanced Correction) - 8.4275 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)