Final Magnetic Moment2.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFiM |
Formation Energy / Atom-2.215 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom1.035 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. |
Density4.19 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLiCrO2 + Li4CrFe3O8 |
Band Gap1.292 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 MauguinI4m2 [119] |
HallI 4 2 |
Point Group42m |
Crystal Systemtetragonal |
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) | <1 1 1> | <0 0 1> | 249.7 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 233.1 |
AlN (mp-661) | <1 0 0> | <1 1 1> | 107.4 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 199.8 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 199.8 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 299.7 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 199.8 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 180.4 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 299.7 |
SiO2 (mp-6930) | <1 1 0> | <1 0 0> | 144.4 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 83.2 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 149.8 |
CeO2 (mp-20194) | <1 1 0> | <1 1 1> | 214.7 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 33.3 |
GaAs (mp-2534) | <1 1 0> | <1 0 0> | 144.4 |
GaAs (mp-2534) | <1 1 1> | <1 0 0> | 288.7 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 153.1 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 133.2 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 144.4 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 166.5 |
InAs (mp-20305) | <1 1 0> | <1 0 0> | 108.3 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 83.2 |
BaF2 (mp-1029) | <1 1 0> | <1 0 0> | 108.3 |
ZnSe (mp-1190) | <1 1 0> | <1 0 0> | 144.4 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 116.5 |
CdS (mp-672) | <0 0 1> | <1 0 0> | 360.9 |
CdS (mp-672) | <1 0 1> | <1 0 1> | 238.5 |
LiF (mp-1138) | <1 1 1> | <1 0 1> | 278.2 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 316.3 |
GaN (mp-804) | <0 0 1> | <1 0 1> | 318.0 |
GaN (mp-804) | <1 0 0> | <1 0 1> | 198.7 |
GaN (mp-804) | <1 1 0> | <1 0 1> | 318.0 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 249.7 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 216.4 |
YVO4 (mp-19133) | <1 0 1> | <1 0 1> | 278.2 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 255.2 |
SiO2 (mp-6930) | <1 1 1> | <1 0 0> | 108.3 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 349.6 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 149.8 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 288.7 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 1> | 159.0 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 66.6 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 149.8 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 33.3 |
ZnSe (mp-1190) | <1 1 1> | <1 0 0> | 288.7 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 16.6 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 266.4 |
GaSe (mp-1943) | <1 0 0> | <1 1 0> | 204.2 |
GaSe (mp-1943) | <1 0 1> | <1 1 0> | 204.2 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 83.2 |
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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Piezoelectric Tensor eij (C/m2) |
|||||
---|---|---|---|---|---|
0.00000 | 0.00000 | 0.00000 | 0.00000 | -0.09786 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | 0.09786 | 0.00000 | 0.00000 |
-0.66638 | 0.66638 | 0.00000 | 0.00000 | 0.00000 | 0.00000 |
Piezoelectric Modulus ‖eij‖max0.94240 C/m2 |
Crystallographic Direction vmax |
---|
0.00000 |
1.00000 |
0.00000 |
Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
5.19 | 0.00 | 0.00 |
0.00 | 5.19 | 0.00 |
0.00 | 0.00 | 4.99 |
Dielectric Tensor εij (total) |
||
---|---|---|
16.66 | 0.00 | 0.00 |
0.00 | 16.66 | 0.00 |
0.00 | 0.00 | 42.01 |
Polycrystalline dielectric constant
εpoly∞
5.13
|
Polycrystalline dielectric constant
εpoly
25.11
|
Refractive Index n2.26 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
LiFeO2 (mp-18782) | 0.1542 | 0.020 | 3 |
LiCrO2 (mp-762454) | 0.0271 | 0.038 | 3 |
NaYbO2 (mp-756878) | 0.1451 | 0.098 | 3 |
LiInO2 (mp-5488) | 0.1378 | 0.000 | 3 |
Ca2NF (mp-33588) | 0.1231 | 0.030 | 3 |
Li2VCrO4 (mp-775047) | 0.1042 | 0.036 | 4 |
Li2MnCrO4 (mp-773308) | 0.0400 | 0.035 | 4 |
Li2CrNiO4 (mp-773255) | 0.1547 | 0.073 | 4 |
Li2CrCoO4 (mp-770000) | 0.1271 | 0.103 | 4 |
Li2CoNiO4 (mp-761608) | 0.1285 | 0.088 | 4 |
Te2Au (mp-1662) | 0.6388 | 0.018 | 2 |
NaTe3 (mp-28478) | 0.4393 | 0.000 | 2 |
LiTe3 (mp-27466) | 0.5823 | 0.009 | 2 |
BaO (mp-776658) | 0.7021 | 0.019 | 2 |
Te2Au (mp-567525) | 0.6100 | 0.018 | 2 |
Na6MnNi3(SbO6)2 (mp-1094109) | 0.6899 | 0.005 | 5 |
Te (mp-570459) | 0.7465 | 0.044 | 1 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesCr: 3.7 eVFe: 5.3 eV |
PseudopotentialsVASP PAW: Li_sv Cr_pv Fe_pv O |
Final Energy/Atom-6.4876 eV |
Corrected Energy-59.4556 eV
-59.4556 eV = -51.9004 eV (uncorrected energy) - 4.7460 eV (MP Advanced Correction) - 2.8092 eV (MP Anion Correction)
|
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)