Final Magnetic Moment0.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingAFM |
Formation Energy / Atom-1.837 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 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. |
Density5.14 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap1.592 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 MauguinImma [74] |
Hall-I 2b 2 |
Point Groupmmm |
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] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <0 0 1> | 262.8 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 112.6 |
AlN (mp-661) | <1 0 1> | <0 1 1> | 128.1 |
AlN (mp-661) | <1 1 0> | <0 1 0> | 311.3 |
AlN (mp-661) | <1 1 1> | <0 1 0> | 207.5 |
CeO2 (mp-20194) | <1 0 0> | <1 1 0> | 148.8 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 337.9 |
GaAs (mp-2534) | <1 0 0> | <1 1 0> | 297.5 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 159.9 |
BaF2 (mp-1029) | <1 1 0> | <0 0 1> | 112.6 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 225.3 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 187.7 |
GaN (mp-804) | <1 0 1> | <0 1 0> | 259.4 |
GaN (mp-804) | <1 1 0> | <0 1 0> | 311.3 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 150.2 |
SiO2 (mp-6930) | <0 0 1> | <1 1 0> | 223.1 |
SiO2 (mp-6930) | <1 1 1> | <0 1 1> | 256.2 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 159.9 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 112.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 1> | 249.9 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 225.3 |
DyScO3 (mp-31120) | <0 1 1> | <0 1 1> | 320.2 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 37.5 |
InAs (mp-20305) | <1 1 0> | <0 1 0> | 51.9 |
InAs (mp-20305) | <1 1 1> | <0 1 0> | 259.4 |
ZnSe (mp-1190) | <1 0 0> | <1 1 0> | 297.5 |
KTaO3 (mp-3614) | <1 0 0> | <1 1 0> | 148.8 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 0> | 207.5 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 337.9 |
CdS (mp-672) | <1 0 0> | <1 0 1> | 260.8 |
CdS (mp-672) | <1 0 1> | <0 1 0> | 259.4 |
LiF (mp-1138) | <1 0 0> | <1 1 0> | 148.8 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 207.5 |
Te2W (mp-22693) | <0 0 1> | <1 0 1> | 65.2 |
Te2W (mp-22693) | <0 1 0> | <1 1 1> | 166.6 |
Te2W (mp-22693) | <0 1 1> | <1 1 0> | 297.5 |
Te2W (mp-22693) | <1 0 0> | <0 0 1> | 187.7 |
Te2W (mp-22693) | <1 0 1> | <1 0 1> | 195.6 |
YVO4 (mp-19133) | <0 0 1> | <0 1 1> | 320.2 |
YVO4 (mp-19133) | <1 0 0> | <0 0 1> | 225.3 |
YVO4 (mp-19133) | <1 1 0> | <1 0 1> | 65.2 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 337.9 |
Te2Mo (mp-602) | <0 0 1> | <1 0 1> | 65.2 |
Te2Mo (mp-602) | <1 0 0> | <0 1 1> | 320.2 |
Te2Mo (mp-602) | <1 0 1> | <0 1 1> | 320.2 |
Te2Mo (mp-602) | <1 1 0> | <0 0 1> | 187.7 |
Te2Mo (mp-602) | <1 1 1> | <0 0 1> | 187.7 |
Ag (mp-124) | <1 0 0> | <0 1 1> | 256.2 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 75.1 |
Ag (mp-124) | <1 1 1> | <0 0 1> | 187.7 |
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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Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
3.96 | -0.00 | 0.00 |
-0.00 | 3.69 | -0.00 |
0.00 | -0.00 | 3.38 |
Dielectric Tensor εij (total) |
||
---|---|---|
10.57 | -0.00 | 0.00 |
-0.00 | 7.55 | -0.00 |
0.00 | -0.00 | 7.56 |
Polycrystalline dielectric constant
εpoly∞
3.68
|
Polycrystalline dielectric constant
εpoly
8.56
|
Refractive Index n1.92 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Fe(CoO2)2 (mp-767034) | 0.1137 | 0.017 | 3 |
MgMn2O4 (mvc-6916) | 0.1293 | 0.047 | 3 |
Co2SnO4 (mp-691116) | 0.1308 | 0.000 | 3 |
Mn2NiO4 (mp-690523) | 0.1274 | 0.012 | 3 |
Mg2TcO4 (mp-34433) | 0.1039 | 0.053 | 3 |
LiCoSbO4 (mp-773544) | 0.1299 | 0.000 | 4 |
LiNbNiO4 (mp-772247) | 0.1153 | 0.067 | 4 |
Li2Fe3SbO8 (mp-776233) | 0.1283 | 0.008 | 4 |
Li2NbFe3O8 (mp-776115) | 0.1258 | 0.047 | 4 |
LiFeSnO4 (mp-771096) | 0.1157 | 0.001 | 4 |
Hf3N4 (mp-755988) | 0.2179 | 0.016 | 2 |
Zr3N4 (mp-754381) | 0.2196 | 0.035 | 2 |
In3S4 (mp-556597) | 0.1869 | 0.042 | 2 |
Sn3N4 (mp-16031) | 0.1943 | 0.000 | 2 |
Ge3N4 (mp-476) | 0.2101 | 0.109 | 2 |
Li4Cr2Fe3Co3O16 (mp-775698) | 0.3048 | 0.894 | 5 |
Li14Mn22Cr3Cu3O56 (mp-735790) | 0.2934 | 0.019 | 5 |
Li4Mn3Cr3(CuO8)2 (mp-765456) | 0.2790 | 0.080 | 5 |
Li4Cr3Cu3(SbO8)2 (mp-783908) | 0.2981 | 0.040 | 5 |
Li4Fe3Co3(TeO8)2 (mp-849468) | 0.3063 | 0.064 | 5 |
Li3MnFeCo(PO4)3 (mp-764809) | 0.7256 | 0.015 | 6 |
Li3MnFeCo(PO4)3 (mp-764869) | 0.7312 | 0.032 | 6 |
Li3MnFeCo(PO4)3 (mp-764707) | 0.7345 | 0.035 | 6 |
Li3MnFeCo(PO4)3 (mp-764969) | 0.7283 | 0.032 | 6 |
Li3MnFeCo(PO4)3 (mp-764870) | 0.7333 | 0.661 | 6 |
Run TypeGGA+U |
Energy Cutoff700 eV |
# of K-pointsNone |
U ValuesNi: 6.2 eV |
PseudopotentialsVASP PAW: Li_sv Ni_pv Sb O |
Final Energy/Atom-5.6423 eV |
Corrected Energy-177.8772 eV
-177.8772 eV = -157.9846 eV (uncorrected energy) - 11.2366 eV (MP Anion Correction) - 8.6560 eV (MP Advanced 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)