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 OrderingUnknown |
Formation Energy / Atom-0.698 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. |
Density8.31 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.014 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 MauguinC2221 [20] |
HallC 2c 2 |
Point Group222 |
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%)
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| substrate material | substrate orientation | film orientation | MCIA† [Å2] |
|---|---|---|---|
| Al (mp-134) | <1 1 0> | <0 0 1> | 158.0 |
| AlN (mp-661) | <0 0 1> | <0 0 1> | 315.9 |
| AlN (mp-661) | <1 0 1> | <0 0 1> | 158.0 |
| TeO2 (mp-2125) | <0 0 1> | <0 0 1> | 158.0 |
| TeO2 (mp-2125) | <0 1 1> | <0 0 1> | 79.0 |
| TeO2 (mp-2125) | <1 0 1> | <0 0 1> | 79.0 |
| GaAs (mp-2534) | <1 0 0> | <0 0 1> | 236.9 |
| GaAs (mp-2534) | <1 1 0> | <0 0 1> | 236.9 |
| GaN (mp-804) | <1 0 0> | <0 0 1> | 236.9 |
| GaN (mp-804) | <1 1 0> | <0 0 1> | 236.9 |
| DyScO3 (mp-31120) | <0 0 1> | <0 0 1> | 158.0 |
| DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 315.9 |
| ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 236.9 |
| ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 236.9 |
| KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 158.0 |
| C (mp-66) | <1 0 0> | <0 0 1> | 315.9 |
| CdS (mp-672) | <1 0 0> | <0 0 1> | 236.9 |
| GdScO3 (mp-5690) | <0 0 1> | <0 0 1> | 158.0 |
| GdScO3 (mp-5690) | <1 0 0> | <0 0 1> | 236.9 |
| GdScO3 (mp-5690) | <1 1 0> | <0 0 1> | 315.9 |
| LiF (mp-1138) | <1 0 0> | <0 0 1> | 236.9 |
| LiF (mp-1138) | <1 1 0> | <0 0 1> | 236.9 |
| Mg (mp-153) | <1 0 0> | <0 0 1> | 236.9 |
| Ag (mp-124) | <1 1 0> | <0 0 1> | 315.9 |
| Ag (mp-124) | <1 1 1> | <0 0 1> | 236.9 |
| TbScO3 (mp-31119) | <0 0 1> | <0 0 1> | 158.0 |
| TbScO3 (mp-31119) | <1 0 0> | <0 0 1> | 315.9 |
| Ni (mp-23) | <1 0 0> | <0 0 1> | 236.9 |
| BaTiO3 (mp-5986) | <1 0 0> | <0 0 1> | 315.9 |
| BaTiO3 (mp-5986) | <1 1 0> | <0 0 1> | 236.9 |
| BaTiO3 (mp-5986) | <1 1 1> | <0 0 1> | 236.9 |
| NdGaO3 (mp-3196) | <0 0 1> | <0 0 1> | 158.0 |
| NdGaO3 (mp-3196) | <1 0 0> | <0 0 1> | 315.9 |
| Au (mp-81) | <1 1 0> | <0 0 1> | 315.9 |
| Au (mp-81) | <1 1 1> | <0 0 1> | 236.9 |
| Ga2O3 (mp-886) | <1 0 0> | <0 0 1> | 236.9 |
| ZrO2 (mp-2858) | <0 1 0> | <0 0 1> | 315.9 |
| NaCl (mp-22862) | <1 1 0> | <0 0 1> | 236.9 |
| ZnO (mp-2133) | <1 1 0> | <0 0 1> | 236.9 |
| MgF2 (mp-1249) | <1 0 1> | <0 0 1> | 79.0 |
| Ge (mp-32) | <1 1 0> | <0 0 1> | 236.9 |
| LiAlO2 (mp-3427) | <1 0 0> | <0 0 1> | 236.9 |
| SrTiO3 (mp-4651) | <1 1 0> | <0 0 1> | 315.9 |
| Ge (mp-32) | <1 0 0> | <0 0 1> | 236.9 |
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 |
|---|---|---|---|
| Tb3Ge5 (mp-2321) | 0.3428 | 0.000 | 2 |
| Y3Ge5 (mp-17118) | 0.3250 | 0.000 | 2 |
| Dy3Ge5 (mp-505577) | 0.3185 | 0.000 | 2 |
| Ho3Ge5 (mp-542748) | 0.3587 | 0.000 | 2 |
| Sm3Ge5 (mp-580126) | 0.4043 | 0.009 | 2 |
| K2HfF6 (mp-14128) | 0.6003 | 0.000 | 3 |
| BaCaSn3 (mp-583645) | 0.5973 | 0.000 | 3 |
| YbBaSn3 (mp-571479) | 0.5796 | 0.000 | 3 |
| CsU2F9 (mp-39066) | 0.4921 | 0.004 | 3 |
| Sm3Si2Ni (mp-617312) | 0.5898 | 0.000 | 3 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-points11 |
U Values-- |
PseudopotentialsVASP PAW: Ge_d Ho_3 |
Final Energy/Atom-5.3050 eV |
Corrected Energy-392.5685 eV
-392.5685 eV = -392.5685 eV (uncorrected energy)
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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)