Final Magnetic Moment23.011 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-1.796 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.897 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. |
Density4.51 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCrCoO4 + CoO2 + Li4CrFe3O8 |
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 MauguinCm [8] |
HallC 2y |
Point Groupm |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <0 1 0> | 93.6 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 108.1 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 162.2 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 229.9 |
AlN (mp-661) | <0 0 1> | <1 0 0> | 270.3 |
AlN (mp-661) | <1 1 0> | <0 1 1> | 109.8 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 115.0 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 324.4 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 324.4 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 172.5 |
SiO2 (mp-6930) | <1 0 0> | <0 1 1> | 109.8 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 280.7 |
GaN (mp-804) | <1 0 0> | <1 0 1> | 237.7 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 1> | 158.4 |
DyScO3 (mp-31120) | <0 1 1> | <0 1 1> | 109.8 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 229.9 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 324.4 |
DyScO3 (mp-31120) | <1 1 1> | <0 1 1> | 219.6 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 162.2 |
ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 229.9 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 162.2 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 115.0 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 57.5 |
CdS (mp-672) | <1 0 0> | <1 0 1> | 237.7 |
LiF (mp-1138) | <1 0 0> | <1 0 1> | 237.7 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 115.0 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 57.5 |
YVO4 (mp-19133) | <1 0 1> | <1 0 0> | 270.3 |
YVO4 (mp-19133) | <1 1 0> | <0 1 0> | 187.1 |
TePb (mp-19717) | <1 1 0> | <0 1 0> | 187.1 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 172.5 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 172.5 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 57.5 |
BN (mp-984) | <0 0 1> | <0 0 1> | 115.0 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 115.0 |
Al (mp-134) | <1 1 0> | <0 0 1> | 115.0 |
LiGaO2 (mp-5854) | <0 1 1> | <0 0 1> | 172.5 |
LiGaO2 (mp-5854) | <1 0 0> | <0 1 0> | 280.7 |
CdTe (mp-406) | <1 1 0> | <0 1 0> | 187.1 |
TeO2 (mp-2125) | <0 1 0> | <1 0 0> | 216.3 |
C (mp-66) | <1 1 0> | <0 1 1> | 109.8 |
C (mp-66) | <1 1 1> | <0 0 1> | 172.5 |
GdScO3 (mp-5690) | <1 1 0> | <1 0 1> | 316.9 |
GdScO3 (mp-5690) | <1 1 1> | <0 1 1> | 219.6 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 115.0 |
Mg (mp-153) | <1 1 1> | <1 0 0> | 324.4 |
Al (mp-134) | <1 0 0> | <1 0 0> | 162.2 |
Al (mp-134) | <1 1 1> | <0 0 1> | 57.5 |
LiGaO2 (mp-5854) | <0 0 1> | <0 1 1> | 109.8 |
CdTe (mp-406) | <1 0 0> | <1 0 0> | 270.3 |
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 |
---|---|---|---|
Li(CoO2)2 (mp-771481) | 0.1971 | 0.136 | 3 |
Li(FeO2)2 (mp-771571) | 0.0851 | 0.665 | 3 |
LiCr2O4 (mp-771523) | 0.1591 | 0.088 | 3 |
Li(NiO2)2 (mp-771429) | 0.1906 | 0.063 | 3 |
LiTi2O4 (mp-776170) | 0.1564 | 0.042 | 3 |
Li4Mn3Cr5O16 (mp-771517) | 0.0966 | 0.039 | 4 |
Li4Mn5Cr3O16 (mp-772402) | 0.0844 | 0.054 | 4 |
Li2Cr3FeO8 (mp-775335) | 0.0913 | 0.877 | 4 |
Li4Ti3V5O16 (mp-777694) | 0.1105 | 0.073 | 4 |
Li4Cr3Fe5O16 (mp-772464) | 0.1065 | 0.899 | 4 |
Fe3O4 (mp-715491) | 0.3270 | 0.017 | 2 |
Fe3O4 (mp-542433) | 0.3344 | 0.075 | 2 |
Cr3N4 (mp-1014358) | 0.3032 | 0.226 | 2 |
Fe3O4 (mp-650112) | 0.3111 | 0.060 | 2 |
Fe3O4 (mp-31770) | 0.3510 | 0.017 | 2 |
Li4Mn2Fe3Co3O16 (mp-761441) | 0.0922 | 0.078 | 5 |
Li4Mn3Cr3(FeO8)2 (mp-761449) | 0.0917 | 0.570 | 5 |
Li4Ti3Fe3(CuO8)2 (mp-763962) | 0.1029 | 6.078 | 5 |
Li4Cr3Fe2Co3O16 (mp-763763) | 0.0843 | 0.614 | 5 |
Li4Mn3Cr2Fe3O16 (mp-849471) | 0.0896 | 0.852 | 5 |
Li3MnFeCo(PO4)3 (mp-764931) | 0.6934 | 0.017 | 6 |
Li3MnFeCo(PO4)3 (mp-764809) | 0.6834 | 0.014 | 6 |
Li3MnFeCo(PO4)3 (mp-764869) | 0.6872 | 0.032 | 6 |
Li3MnFeCo(PO4)3 (mp-764969) | 0.6887 | 0.057 | 6 |
Li3MnFeCo(PO4)3 (mp-764870) | 0.6912 | 0.466 | 6 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesCr: 3.7 eVFe: 5.3 eV Co: 3.32 eV |
PseudopotentialsVASP PAW: Li_sv Cr_pv Fe_pv Co O |
Final Energy/Atom-6.2159 eV |
Corrected Energy-200.7185 eV
Uncorrected energy = -174.0465 eV
Composition-based energy adjustment (-0.687 eV/atom x 16.0 atoms) = -10.9920 eV
Composition-based energy adjustment (-1.999 eV/atom x 2.0 atoms) = -3.9980 eV
Composition-based energy adjustment (-2.256 eV/atom x 3.0 atoms) = -6.7680 eV
Composition-based energy adjustment (-1.638 eV/atom x 3.0 atoms) = -4.9140 eV
Corrected energy = -200.7185 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)