Final Magnetic Moment0.001 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-2.203 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.212 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. |
Density2.78 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLi2FeO3 + LiAlO2 |
Band Gap0.206 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 MauguinPna21 [33] |
HallP 2c 2n |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 86.6 |
DyScO3 (mp-31120) | <0 1 1> | <0 0 1> | 54.1 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 259.9 |
InAs (mp-20305) | <1 1 1> | <0 1 1> | 259.7 |
KTaO3 (mp-3614) | <1 0 0> | <1 1 1> | 245.0 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 216.4 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 324.6 |
CdS (mp-672) | <1 0 1> | <0 1 1> | 259.7 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 351.7 |
Te2W (mp-22693) | <0 1 0> | <0 1 1> | 259.7 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 243.5 |
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 216.4 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 297.6 |
LaAlO3 (mp-2920) | <1 1 0> | <0 0 1> | 243.5 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 259.9 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 243.5 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 351.7 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 135.3 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 81.2 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 243.5 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 27.1 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 324.6 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 270.5 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 81.2 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 351.7 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 216.4 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 270.5 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 259.9 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 297.6 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 270.5 |
BN (mp-984) | <0 0 1> | <0 0 1> | 243.5 |
BN (mp-984) | <1 0 1> | <0 0 1> | 81.2 |
LiNbO3 (mp-3731) | <0 0 1> | <0 0 1> | 189.4 |
LiNbO3 (mp-3731) | <1 0 0> | <0 0 1> | 297.6 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 324.6 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 135.3 |
GaN (mp-804) | <1 0 1> | <1 0 1> | 272.3 |
GaN (mp-804) | <1 1 0> | <1 0 0> | 86.6 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 189.4 |
SiO2 (mp-6930) | <0 0 1> | <0 1 1> | 86.6 |
SiO2 (mp-6930) | <1 0 0> | <0 1 0> | 82.2 |
SiO2 (mp-6930) | <1 0 1> | <0 0 1> | 351.7 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 297.6 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 243.5 |
Al (mp-134) | <1 0 0> | <1 1 1> | 245.0 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 243.5 |
DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 189.4 |
Al (mp-134) | <1 1 0> | <0 0 1> | 216.4 |
Al (mp-134) | <1 1 1> | <0 0 1> | 324.6 |
LiGaO2 (mp-5854) | <0 0 1> | <0 0 1> | 27.1 |
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 |
---|---|---|---|
MgGeN2 (mp-7798) | 0.1941 | 0.000 | 3 |
MnGeN2 (mp-20692) | 0.1744 | 0.124 | 3 |
ZnSiN2 (mp-1020712) | 0.1998 | 0.000 | 3 |
Zn2CrN3 (mp-1029458) | 0.1719 | 0.000 | 3 |
MnZn2N3 (mp-1029354) | 0.1882 | 0.006 | 3 |
Li4TiMn3O8 (mp-771622) | 0.2078 | 0.103 | 4 |
Li3AlCrO5 (mp-770586) | 0.2023 | 0.091 | 4 |
Li2AlCoO4 (mp-770553) | 0.1976 | 0.211 | 4 |
Li2AlNiO4 (mp-770357) | 0.1966 | 0.165 | 4 |
Li4NbFe3O8 (mp-773248) | 0.2122 | 0.056 | 4 |
CdP2 (mp-913) | 0.3251 | 0.000 | 2 |
ZnP2 (mp-2782) | 0.2672 | 0.000 | 2 |
ZnP2 (mp-11025) | 0.2685 | 0.000 | 2 |
ZnP2 (mp-1392) | 0.3309 | 0.004 | 2 |
CdP2 (mp-12112) | 0.3253 | 0.000 | 2 |
Si (mp-971662) | 0.5106 | 0.064 | 1 |
Si (mp-1079297) | 0.4879 | 0.074 | 1 |
C (mp-1078845) | 0.3948 | 0.266 | 1 |
C (mp-1080826) | 0.4459 | 0.299 | 1 |
Si (mp-1095269) | 0.4901 | 0.096 | 1 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesFe: 5.3 eV |
PseudopotentialsVASP PAW: Li_sv Al Fe_pv O |
Final Energy/Atom-5.8469 eV |
Corrected Energy-258.8552 eV
-258.8552 eV = -233.8774 eV (uncorrected energy) - 14.0458 eV (MP Anion Correction) - 10.9320 eV (MP Advanced 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)