Final Magnetic Moment48.995 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-1.900 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.043 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. |
Density4.81 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLiFeO2 + FeO |
Band Gap0.368 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 [1] |
HallP 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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 220.7 |
LaAlO3 (mp-2920) | <1 0 0> | <1 -1 1> | 215.0 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 220.7 |
AlN (mp-661) | <1 1 1> | <0 1 -1> | 144.7 |
CeO2 (mp-20194) | <1 0 0> | <0 1 -1> | 144.7 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 220.7 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 220.7 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 283.7 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 220.7 |
SiO2 (mp-6930) | <0 0 1> | <0 1 -1> | 217.1 |
SiO2 (mp-6930) | <1 0 1> | <1 0 0> | 302.9 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 189.1 |
InAs (mp-20305) | <1 1 0> | <1 1 -1> | 158.1 |
ZnSe (mp-1190) | <1 0 0> | <0 1 -1> | 289.4 |
KTaO3 (mp-3614) | <1 0 0> | <0 1 -1> | 144.7 |
KTaO3 (mp-3614) | <1 1 0> | <1 -1 0> | 206.0 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 283.7 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 252.2 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 157.6 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 220.7 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 157.6 |
GaSe (mp-1943) | <0 0 1> | <0 1 -1> | 289.4 |
BN (mp-984) | <0 0 1> | <1 0 -1> | 218.8 |
BN (mp-984) | <1 0 0> | <1 0 -1> | 291.7 |
BN (mp-984) | <1 0 1> | <0 1 -1> | 217.1 |
AlN (mp-661) | <0 0 1> | <1 1 -1> | 316.2 |
AlN (mp-661) | <1 0 0> | <1 -1 0> | 206.0 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 126.1 |
AlN (mp-661) | <1 1 0> | <0 1 1> | 316.9 |
GaAs (mp-2534) | <1 0 0> | <0 1 -1> | 289.4 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 220.7 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 220.7 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 283.7 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 220.7 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 220.7 |
CdS (mp-672) | <1 0 1> | <1 0 -1> | 291.7 |
CdS (mp-672) | <1 1 0> | <0 1 0> | 301.3 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 346.7 |
Te2W (mp-22693) | <0 1 0> | <1 1 0> | 315.9 |
Te2W (mp-22693) | <0 1 1> | <0 1 -1> | 289.4 |
Te2Mo (mp-602) | <0 0 1> | <0 1 -1> | 217.1 |
Te2Mo (mp-602) | <1 0 0> | <1 1 0> | 315.9 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 283.7 |
Te2Mo (mp-602) | <1 1 0> | <1 1 0> | 189.6 |
Te2Mo (mp-602) | <1 1 1> | <0 0 1> | 94.6 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 126.1 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 31.5 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 126.1 |
LiNbO3 (mp-3731) | <0 0 1> | <0 0 1> | 94.6 |
LiNbO3 (mp-3731) | <1 0 1> | <1 1 0> | 315.9 |
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 |
---|---|---|---|
Li5Fe7O12 (mp-771531) | 0.1295 | 0.025 | 3 |
Li9Fe23O32 (mp-773975) | 0.1352 | 0.036 | 3 |
LiCoO2 (mp-853240) | 0.1345 | 0.075 | 3 |
Li5V7O12 (mp-764746) | 0.1119 | 0.369 | 3 |
LiCoO2 (mp-1097885) | 0.1370 | 0.103 | 3 |
Li5Fe5(NiO6)2 (mp-771555) | 0.1065 | 0.027 | 4 |
Li4Cr3NiO8 (mp-769719) | 0.1058 | 0.023 | 4 |
Li4Cr3NiO8 (mp-770297) | 0.1140 | 0.250 | 4 |
Li3CoOF3 (mp-764000) | 0.1158 | 0.224 | 4 |
Li4Cr3NiO8 (mp-770046) | 0.1025 | 0.017 | 4 |
LiTe3 (mp-27466) | 0.2441 | 0.009 | 2 |
Bi2Te3 (mp-568390) | 0.2915 | 0.248 | 2 |
In2Se3 (mp-1068548) | 0.2751 | 0.530 | 2 |
In2Se3 (mp-20830) | 0.2602 | 0.530 | 2 |
Sb2Te3 (mp-1080789) | 0.2859 | 0.129 | 2 |
Na6MnNi3(SbO6)2 (mp-1094109) | 0.5347 | 0.139 | 5 |
Hg (mp-982872) | 0.4514 | 0.020 | 1 |
Sb (mp-632286) | 0.4062 | 0.059 | 1 |
Te (mp-570459) | 0.4560 | 0.044 | 1 |
Te (mp-10654) | 0.4811 | 0.047 | 1 |
Te (mp-105) | 0.3775 | 0.047 | 1 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesFe: 5.3 eV |
PseudopotentialsVASP PAW: Li_sv Fe_pv O |
Final Energy/Atom-6.2934 eV |
Corrected Energy-242.6883 eV
-242.6883 eV = -201.3886 eV (uncorrected energy) - 30.0630 eV (MP Advanced Correction) - 11.2366 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)