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-0.678 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. |
Density11.72 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 |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
Fe3O4 (mp-19306) | <1 1 0> | <1 1 0> | 199.0 |
MgO (mp-1265) | <1 0 0> | <1 0 0> | 93.8 |
MgO (mp-1265) | <1 1 0> | <1 1 0> | 199.0 |
TiO2 (mp-2657) | <0 0 1> | <1 0 0> | 187.6 |
Ge3(BiO3)4 (mp-23560) | <1 0 0> | <1 0 0> | 234.5 |
C (mp-66) | <1 0 0> | <1 0 0> | 234.5 |
C (mp-66) | <1 1 0> | <1 1 0> | 199.0 |
GdScO3 (mp-5690) | <0 1 1> | <1 1 1> | 162.5 |
GdScO3 (mp-5690) | <1 0 1> | <1 0 0> | 281.4 |
Mg (mp-153) | <0 0 1> | <1 0 0> | 234.5 |
Mg (mp-153) | <1 1 0> | <1 1 0> | 265.3 |
Mg (mp-153) | <1 1 1> | <1 0 0> | 234.5 |
KP(HO2)2 (mp-23959) | <1 0 0> | <1 0 0> | 234.5 |
PbS (mp-21276) | <1 0 0> | <1 0 0> | 187.6 |
PbS (mp-21276) | <1 1 0> | <1 1 0> | 199.0 |
PbS (mp-21276) | <1 1 1> | <1 1 1> | 243.7 |
GaP (mp-2490) | <1 0 0> | <1 0 0> | 234.5 |
GaP (mp-2490) | <1 1 0> | <1 1 0> | 132.7 |
GaP (mp-2490) | <1 1 1> | <1 1 0> | 265.3 |
InP (mp-20351) | <1 0 0> | <1 0 0> | 187.6 |
InP (mp-20351) | <1 1 0> | <1 1 0> | 199.0 |
InP (mp-20351) | <1 1 1> | <1 1 1> | 243.7 |
TbScO3 (mp-31119) | <0 1 1> | <1 1 1> | 162.5 |
TbScO3 (mp-31119) | <1 0 1> | <1 0 0> | 281.4 |
Ni (mp-23) | <1 0 0> | <1 1 1> | 243.7 |
Ni (mp-23) | <1 1 0> | <1 1 1> | 243.7 |
Ni (mp-23) | <1 1 1> | <1 0 0> | 328.3 |
PbSe (mp-2201) | <1 0 0> | <1 0 0> | 187.6 |
BaTiO3 (mp-5986) | <0 0 1> | <1 1 0> | 331.7 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 331.7 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 234.5 |
NdGaO3 (mp-3196) | <0 1 0> | <1 1 0> | 132.7 |
NdGaO3 (mp-3196) | <0 1 1> | <1 1 1> | 162.5 |
NdGaO3 (mp-3196) | <1 0 1> | <1 1 1> | 162.5 |
NdGaO3 (mp-3196) | <1 1 0> | <1 0 0> | 234.5 |
SiC (mp-11714) | <0 0 1> | <1 0 0> | 328.3 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 132.7 |
CeO2 (mp-20194) | <1 1 1> | <1 1 0> | 265.3 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 132.7 |
GaAs (mp-2534) | <1 1 1> | <1 0 0> | 281.4 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 187.6 |
GaN (mp-804) | <0 0 1> | <1 1 1> | 81.2 |
GaN (mp-804) | <1 1 0> | <1 1 0> | 265.3 |
SiC (mp-11714) | <1 0 1> | <1 0 0> | 328.3 |
Ga2O3 (mp-886) | <1 0 -1> | <1 0 0> | 187.6 |
Si (mp-149) | <1 0 0> | <1 0 0> | 234.5 |
SiO2 (mp-6930) | <1 0 0> | <1 1 0> | 331.7 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 1> | 162.5 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 1> | 162.5 |
Si (mp-149) | <1 1 0> | <1 1 0> | 132.7 |
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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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
YbBiPd (mp-30466) | 0.0000 | 0.000 | 3 |
LiMgP (mp-10178) | 0.0000 | 0.351 | 3 |
USbRh (mp-10624) | 0.0000 | 0.014 | 3 |
MnSbRh (mp-4846) | 0.0000 | 0.066 | 3 |
MnSnPt (mp-21418) | 0.0000 | 0.048 | 3 |
NdH2 (mp-24096) | 0.0000 | 0.000 | 2 |
TiF2 (mp-282) | 0.0000 | 0.248 | 2 |
Mg2Sn (mp-2343) | 0.0000 | 0.000 | 2 |
Na2Se (mp-1266) | 0.0000 | 0.000 | 2 |
Si2Ru (mp-12874) | 0.0000 | 0.289 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Dy_3 Pb_d Au |
Final Energy/Atom-4.5426 eV |
Corrected Energy-13.6277 eV
-13.6277 eV = -13.6277 eV (uncorrected energy)
|
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)