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 OrderingNM |
Formation Energy / Atom-0.313 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. |
Density10.16 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
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 MauguinFm3m [225] |
Hall-F 4 2 3 |
Point Groupm3m |
Crystal Systemcubic |
Topological ClassificationSM*
|
SubclassificationES†
|
Crossing TypeLine
|
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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Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <1 1 1> | 74.2 |
LaAlO3 (mp-2920) | <1 0 1> | <1 1 0> | 303.0 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 181.8 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 242.4 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 121.2 |
CeO2 (mp-20194) | <1 1 1> | <1 0 0> | 257.1 |
LaAlO3 (mp-2920) | <1 1 0> | <1 1 0> | 121.2 |
AlN (mp-661) | <0 0 1> | <1 1 0> | 303.0 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 171.4 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 181.8 |
GaAs (mp-2534) | <1 1 1> | <1 1 1> | 222.6 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 342.8 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 299.9 |
GaN (mp-804) | <1 0 1> | <1 1 0> | 303.0 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 214.2 |
KCl (mp-23193) | <1 1 1> | <1 1 1> | 74.2 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 342.8 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 42.8 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 60.6 |
DyScO3 (mp-31120) | <1 0 0> | <1 1 0> | 181.8 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 181.8 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 171.4 |
ZnSe (mp-1190) | <1 1 1> | <1 1 1> | 222.6 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 214.2 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 181.8 |
CdS (mp-672) | <1 1 1> | <1 0 0> | 214.2 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 85.7 |
Te2W (mp-22693) | <0 0 1> | <1 1 0> | 242.4 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 342.8 |
TePb (mp-19717) | <1 0 0> | <1 0 0> | 42.8 |
TePb (mp-19717) | <1 1 0> | <1 1 0> | 60.6 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 214.2 |
YVO4 (mp-19133) | <1 0 0> | <1 1 0> | 242.4 |
TePb (mp-19717) | <1 1 1> | <1 1 1> | 74.2 |
Te2Mo (mp-602) | <0 0 1> | <1 1 1> | 296.8 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 85.7 |
BN (mp-984) | <0 0 1> | <1 0 0> | 214.2 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 1 1> | 222.6 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 128.5 |
BN (mp-984) | <1 0 1> | <1 1 1> | 222.6 |
LiNbO3 (mp-3731) | <0 0 1> | <1 0 0> | 214.2 |
LiGaO2 (mp-5854) | <0 0 1> | <1 1 0> | 242.4 |
LiGaO2 (mp-5854) | <1 0 0> | <1 1 0> | 181.8 |
CdTe (mp-406) | <1 0 0> | <1 0 0> | 42.8 |
MoS2 (mp-1434) | <0 0 1> | <1 0 0> | 214.2 |
Al (mp-134) | <1 0 0> | <1 0 0> | 214.2 |
Al (mp-134) | <1 1 0> | <1 1 0> | 181.8 |
LiGaO2 (mp-5854) | <0 1 0> | <1 0 0> | 171.4 |
LiGaO2 (mp-5854) | <1 1 0> | <1 1 0> | 242.4 |
CdTe (mp-406) | <1 1 1> | <1 1 1> | 74.2 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
178 | 35 | 35 | 0 | 0 | 0 |
35 | 178 | 35 | 0 | 0 | 0 |
35 | 35 | 178 | 0 | 0 | 0 |
0 | 0 | 0 | 83 | 0 | 0 |
0 | 0 | 0 | 0 | 83 | 0 |
0 | 0 | 0 | 0 | 0 | 83 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
6 | -1 | -1 | 0 | 0 | 0 |
-1 | 6 | -1 | 0 | 0 | 0 |
-1 | -1 | 6 | 0 | 0 | 0 |
0 | 0 | 0 | 12.1 | 0 | 0 |
0 | 0 | 0 | 0 | 12.1 | 0 |
0 | 0 | 0 | 0 | 0 | 12.1 |
Shear Modulus GV78 GPa |
Bulk Modulus KV82 GPa |
Shear Modulus GR78 GPa |
Bulk Modulus KR82 GPa |
Shear Modulus GVRH78 GPa |
Bulk Modulus KVRH82 GPa |
Elastic Anisotropy0.02 |
Poisson's Ratio0.14 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Mn2CoGe (mp-22289) | 0.0000 | 0.035 | 3 |
TaGaCo2 (mp-30555) | 0.0000 | 0.000 | 3 |
AlVFe2 (mp-5778) | 0.0000 | 0.000 | 3 |
ScAlPd2 (mp-16524) | 0.0000 | 0.000 | 3 |
NbCo2Sn (mp-4583) | 0.0000 | 0.119 | 3 |
LiMgSnPd (mp-7555) | 0.0000 | 0.000 | 4 |
VFeCoGe (mp-1063914) | 0.0000 | 0.000 | 4 |
TiFeCoGe (mp-1018012) | 0.0000 | 0.028 | 4 |
VGaFeCo (mp-1066581) | 0.0000 | 0.029 | 4 |
LiMgSbPd (mp-10179) | 0.0000 | 0.096 | 4 |
Rb3Bi (mp-23304) | 0.0000 | 0.028 | 2 |
LaMg3 (mp-2306) | 0.0000 | 0.063 | 2 |
LiGa (mp-1307) | 0.0000 | 0.000 | 2 |
Li3Hg (mp-1646) | 0.0000 | 0.000 | 2 |
NaTl (mp-1564) | 0.0000 | 0.000 | 2 |
Eu (mp-20071) | 0.0000 | 0.085 | 1 |
Th (mp-11343) | 0.0000 | 0.161 | 1 |
Ba (mp-122) | 0.0000 | 0.000 | 1 |
Np (mp-10207) | 0.0000 | 0.447 | 1 |
Gd (mp-11421) | 0.0000 | 0.088 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Li_sv In_d Ir |
Final Energy/Atom-4.3758 eV |
Corrected Energy-17.5034 eV
Uncorrected energy = -17.5034 eV
Corrected energy = -17.5034 eV
|
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)