Final Magnetic Moment9.000 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-2.366 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.053 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. |
Density3.24 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLi2B4O7 + Fe3BO5 + LiBO2 + Fe2O3 |
Band Gap1.458 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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 0 0> | <0 1 1> | 71.3 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 144.1 |
LaAlO3 (mp-2920) | <1 1 1> | <0 0 1> | 240.2 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 336.3 |
AlN (mp-661) | <1 1 0> | <0 1 1> | 213.8 |
AlN (mp-661) | <1 1 1> | <0 1 1> | 142.5 |
CeO2 (mp-20194) | <1 1 1> | <0 1 1> | 213.8 |
GaAs (mp-2534) | <1 1 1> | <0 1 1> | 285.0 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 240.2 |
BaF2 (mp-1029) | <1 1 0> | <0 0 1> | 288.3 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 144.1 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 336.3 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 240.2 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 336.3 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 144.1 |
SiO2 (mp-6930) | <0 0 1> | <0 0 1> | 288.3 |
SiO2 (mp-6930) | <1 0 0> | <0 1 1> | 213.8 |
SiO2 (mp-6930) | <1 0 1> | <1 0 0> | 274.7 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 240.2 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 288.3 |
KCl (mp-23193) | <1 1 1> | <0 0 1> | 144.1 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 274.7 |
DyScO3 (mp-31120) | <1 1 1> | <1 1 0> | 211.4 |
ZnSe (mp-1190) | <1 1 1> | <0 1 1> | 285.0 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 266.2 |
CdS (mp-672) | <1 0 0> | <0 1 0> | 266.2 |
LiF (mp-1138) | <1 0 0> | <0 1 1> | 285.0 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 211.4 |
Te2W (mp-22693) | <0 0 1> | <0 1 0> | 266.2 |
YVO4 (mp-19133) | <0 0 1> | <1 1 0> | 105.7 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 336.3 |
TePb (mp-19717) | <1 1 0> | <1 0 0> | 183.1 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 144.1 |
Te2Mo (mp-602) | <0 0 1> | <1 1 1> | 230.3 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 288.3 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 336.3 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 0> | 274.7 |
GaSe (mp-1943) | <0 0 1> | <0 1 0> | 319.5 |
GaSe (mp-1943) | <1 0 0> | <1 0 1> | 205.3 |
BN (mp-984) | <0 0 1> | <0 0 1> | 336.3 |
BN (mp-984) | <1 0 0> | <0 1 1> | 213.8 |
BN (mp-984) | <1 0 1> | <0 1 0> | 266.2 |
BN (mp-984) | <1 1 0> | <1 0 0> | 274.7 |
LiNbO3 (mp-3731) | <0 0 1> | <0 0 1> | 48.0 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 288.3 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 336.3 |
Al (mp-134) | <1 0 0> | <0 0 1> | 336.3 |
Al (mp-134) | <1 1 0> | <1 1 0> | 211.4 |
LiGaO2 (mp-5854) | <0 0 1> | <1 0 0> | 274.7 |
LiGaO2 (mp-5854) | <1 1 1> | <0 0 1> | 288.3 |
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 |
---|---|---|---|
Li6B4O9 (mp-768875) | 0.6692 | 0.063 | 3 |
Li6B4O9 (mp-1020024) | 0.7187 | 0.000 | 3 |
LiFe2(BO3)2 (mp-764489) | 0.1252 | 0.462 | 4 |
LiFe2(BO3)2 (mp-764482) | 0.0922 | 0.167 | 4 |
LiFe2(BO3)2 (mp-850256) | 0.1099 | 0.103 | 4 |
LiFe2(BO3)2 (mp-764656) | 0.1210 | 0.049 | 4 |
LiFe2(BO3)2 (mp-764651) | 0.1340 | 0.290 | 4 |
Li4Mn2Fe(BO3)4 (mp-767650) | 0.5552 | 0.319 | 5 |
Li3Mn2Fe(BO3)4 (mp-767643) | 0.7107 | 0.339 | 5 |
Li8MnFe7(BO3)8 (mp-850743) | 0.7157 | 0.017 | 5 |
Li4MnFe2(BO3)4 (mp-767642) | 0.5963 | 0.055 | 5 |
Li8Mn3Fe5(BO3)8 (mp-775252) | 0.7101 | 0.012 | 5 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesFe: 5.3 eV |
PseudopotentialsVASP PAW: Li_sv Fe_pv B O |
Final Energy/Atom-7.1132 eV |
Corrected Energy-351.6985 eV
-351.6985 eV = -312.9795 eV (uncorrected energy) - 21.8640 eV (MP Advanced Correction) - 16.8550 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)