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 OrderingNM |
Formation Energy / Atom-0.568 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. |
Density8.27 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 MauguinF43m [216] |
HallF 4 2 3 |
Point Group43m |
Crystal Systemcubic |
Topological ClassificationSM*
|
SubclassificationESFD†
|
Crossing TypePoint
|
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.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 0 0> | 203.7 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 285.2 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 285.2 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 172.9 |
CeO2 (mp-20194) | <1 1 1> | <1 1 1> | 211.7 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 163.0 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 40.7 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 57.6 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 70.6 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 285.2 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 203.7 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 282.3 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 40.7 |
KCl (mp-23193) | <1 1 0> | <1 1 0> | 57.6 |
KCl (mp-23193) | <1 1 1> | <1 1 1> | 70.6 |
DyScO3 (mp-31120) | <0 1 0> | <1 1 0> | 172.9 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 326.0 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 326.0 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 163.0 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 81.5 |
CdS (mp-672) | <0 0 1> | <1 1 0> | 230.5 |
CdS (mp-672) | <1 1 1> | <1 0 0> | 203.7 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 81.5 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 203.7 |
Te2W (mp-22693) | <1 0 0> | <1 1 0> | 288.1 |
Te2W (mp-22693) | <1 0 1> | <1 0 0> | 203.7 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 203.7 |
YVO4 (mp-19133) | <1 0 0> | <1 1 0> | 230.5 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 326.0 |
TePb (mp-19717) | <1 0 0> | <1 0 0> | 40.7 |
TePb (mp-19717) | <1 1 0> | <1 1 0> | 57.6 |
TePb (mp-19717) | <1 1 1> | <1 1 1> | 70.6 |
Te2Mo (mp-602) | <1 0 0> | <1 1 1> | 282.3 |
Te2Mo (mp-602) | <1 0 1> | <1 1 1> | 282.3 |
Te2Mo (mp-602) | <1 1 0> | <1 1 1> | 282.3 |
Ag (mp-124) | <1 1 1> | <1 1 1> | 211.7 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 0> | 203.7 |
BN (mp-984) | <0 0 1> | <1 1 1> | 70.6 |
LiNbO3 (mp-3731) | <0 0 1> | <1 1 1> | 70.6 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 0> | 230.5 |
MoS2 (mp-1434) | <0 0 1> | <1 0 0> | 285.2 |
Al (mp-134) | <1 0 0> | <1 0 0> | 81.5 |
LiGaO2 (mp-5854) | <0 1 0> | <1 0 0> | 163.0 |
LiGaO2 (mp-5854) | <1 0 0> | <1 1 0> | 172.9 |
LiGaO2 (mp-5854) | <1 1 0> | <1 0 0> | 244.5 |
SiC (mp-7631) | <1 0 0> | <1 1 1> | 141.1 |
SiC (mp-7631) | <1 1 0> | <1 1 0> | 230.5 |
MgO (mp-1265) | <1 0 0> | <1 0 0> | 163.0 |
MgO (mp-1265) | <1 1 0> | <1 1 0> | 230.5 |
TiO2 (mp-2657) | <0 0 1> | <1 0 0> | 203.7 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
76 | 70 | 70 | 0 | 0 | 0 |
70 | 76 | 70 | 0 | 0 | 0 |
70 | 70 | 76 | 0 | 0 | 0 |
0 | 0 | 0 | 43 | 0 | 0 |
0 | 0 | 0 | 0 | 43 | 0 |
0 | 0 | 0 | 0 | 0 | 43 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
100.6 | -48 | -48 | 0 | 0 | 0 |
-48 | 100.6 | -48 | 0 | 0 | 0 |
-48 | -48 | 100.6 | 0 | 0 | 0 |
0 | 0 | 0 | 23.4 | 0 | 0 |
0 | 0 | 0 | 0 | 23.4 | 0 |
0 | 0 | 0 | 0 | 0 | 23.4 |
Shear Modulus GV27 GPa |
Bulk Modulus KV72 GPa |
Shear Modulus GR8 GPa |
Bulk Modulus KR72 GPa |
Shear Modulus GVRH17 GPa |
Bulk Modulus KVRH72 GPa |
Elastic Anisotropy12.92 |
Poisson's Ratio0.39 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Li2AgSn (mp-30350) | 0.0000 | 0.057 | 3 |
Li2CdPb (mp-11305) | 0.0000 | 0.000 | 3 |
ZrCo2Sn (mp-22503) | 0.0000 | 0.016 | 3 |
MnFe2Si (mp-5529) | 0.0000 | 0.000 | 3 |
LiAl2Pd (mp-30817) | 0.0000 | 0.000 | 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 |
LiMgSbPd (mp-10179) | 0.0000 | 0.096 | 4 |
LiMgSnPt (mp-11806) | 0.0000 | 0.000 | 4 |
Li3Tl (mp-7396) | 0.0000 | 0.000 | 2 |
Li3Bi (mp-23222) | 0.0000 | 0.000 | 2 |
BiF3 (mp-23301) | 0.0000 | 0.271 | 2 |
GdMg3 (mp-20534) | 0.0000 | 0.042 | 2 |
Li3Sb (mp-2074) | 0.0000 | 0.000 | 2 |
Eu (mp-20071) | 0.0000 | 0.085 | 1 |
Ce (mp-10024) | 0.0000 | 0.228 | 1 |
Lu (mp-10190) | 0.0000 | 0.132 | 1 |
Np (mp-10207) | 0.0000 | 0.447 | 1 |
Na (mp-127) | 0.0000 | 0.002 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Li_sv In_d Pt |
Final Energy/Atom-3.7284 eV |
Corrected Energy-14.9134 eV
Uncorrected energy = -14.9134 eV
Corrected energy = -14.9134 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)