Final Magnetic Moment1.171 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-2.974 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.014 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. |
Density3.62 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLi2TiO3 + LiTiO2 |
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 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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <0 1 0> | 199.9 |
AlN (mp-661) | <1 0 1> | <0 1 1> | 268.2 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 134.1 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 313.0 |
GaAs (mp-2534) | <1 1 0> | <1 1 1> | 232.7 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 313.0 |
BaF2 (mp-1029) | <1 1 0> | <0 0 1> | 223.5 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 134.1 |
GaN (mp-804) | <1 0 1> | <0 1 1> | 134.1 |
GaN (mp-804) | <1 1 0> | <0 1 0> | 349.9 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 223.5 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 44.7 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 223.5 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 313.0 |
SiO2 (mp-6930) | <1 1 1> | <1 0 1> | 105.1 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 313.0 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 223.5 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 134.1 |
DyScO3 (mp-31120) | <0 1 1> | <0 1 1> | 268.2 |
DyScO3 (mp-31120) | <1 0 1> | <0 1 0> | 349.9 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 223.5 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 223.5 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 134.1 |
ZnSe (mp-1190) | <1 1 0> | <1 1 1> | 232.7 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 1> | 116.4 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 89.4 |
CdS (mp-672) | <1 1 1> | <1 0 0> | 263.5 |
LiF (mp-1138) | <1 1 0> | <1 1 1> | 116.4 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 89.4 |
Te2W (mp-22693) | <0 0 1> | <0 1 0> | 199.9 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 268.2 |
Te2Mo (mp-602) | <1 0 0> | <0 0 1> | 268.2 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 268.2 |
Ag (mp-124) | <1 0 0> | <0 1 0> | 299.9 |
Ag (mp-124) | <1 1 0> | <0 1 1> | 268.2 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 89.4 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 134.1 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 89.4 |
BN (mp-984) | <0 0 1> | <1 0 0> | 87.8 |
BN (mp-984) | <1 0 0> | <0 1 0> | 149.9 |
BN (mp-984) | <1 0 1> | <0 1 0> | 249.9 |
BN (mp-984) | <1 1 0> | <0 0 1> | 134.1 |
BN (mp-984) | <1 1 1> | <0 1 0> | 100.0 |
LiNbO3 (mp-3731) | <0 0 1> | <0 1 0> | 349.9 |
LiNbO3 (mp-3731) | <1 0 1> | <0 1 0> | 149.9 |
MoS2 (mp-1434) | <0 0 1> | <1 0 -1> | 274.8 |
Al (mp-134) | <1 1 0> | <1 1 1> | 116.4 |
Al (mp-134) | <1 1 1> | <0 0 1> | 89.4 |
LiGaO2 (mp-5854) | <0 0 1> | <0 0 1> | 223.5 |
LiGaO2 (mp-5854) | <0 1 0> | <0 0 1> | 134.1 |
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 |
---|---|---|---|
Li2PdO3 (mp-760483) | 0.1511 | 0.000 | 3 |
Li5Fe7O12 (mp-771531) | 0.1591 | 0.025 | 3 |
Li2SnO3 (mp-3540) | 0.1308 | 0.000 | 3 |
Li2PtO3 (mp-531826) | 0.1345 | 0.000 | 3 |
Li2IrO3 (mp-532085) | 0.1409 | 0.000 | 3 |
Li4Cr3CoO8 (mp-770264) | 0.1313 | 0.193 | 4 |
Li4Cr3CoO8 (mp-770255) | 0.1294 | 0.049 | 4 |
Li4Cr3CoO8 (mp-770234) | 0.1294 | 0.247 | 4 |
Li4Cr3NiO8 (mp-770046) | 0.1200 | 0.017 | 4 |
Li4FeCo3O8 (mp-765603) | 0.1201 | 0.122 | 4 |
LiTe3 (mp-27466) | 0.2803 | 0.009 | 2 |
Bi2Te3 (mp-568390) | 0.2711 | 0.248 | 2 |
In2Se3 (mp-1068548) | 0.2540 | 0.530 | 2 |
In2Se3 (mp-20830) | 0.2534 | 0.530 | 2 |
Sb2Te3 (mp-1080789) | 0.2834 | 0.129 | 2 |
Na6MnNi3(SbO6)2 (mp-1094109) | 0.5351 | 0.139 | 5 |
Hg (mp-982872) | 0.4275 | 0.020 | 1 |
Sb (mp-632286) | 0.4628 | 0.059 | 1 |
Se (mp-7755) | 0.4839 | 0.181 | 1 |
Te (mp-10654) | 0.4572 | 0.047 | 1 |
Te (mp-105) | 0.3926 | 0.047 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Li_sv Ti_pv O |
Final Energy/Atom-7.2984 eV |
Corrected Energy-183.5900 eV
-183.5900 eV = -175.1625 eV (uncorrected energy) - 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)