Final Magnetic Moment3.774 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-1.499 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. |
Density8.82 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 MauguinCm [8] |
HallC 2y |
Point Groupm |
Crystal Systemmonoclinic |
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%)
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 |
---|---|---|---|
Rb(ThSe3)2 (mp-9523) | 0.6078 | 0.000 | 3 |
K(ThSe3)2 (mp-9522) | 0.6401 | 0.000 | 3 |
K(USe3)2 (mp-12414) | 0.6409 | 0.000 | 3 |
CsMnP (mp-1077378) | 0.6529 | 0.106 | 3 |
U2TlSe6 (mp-1078777) | 0.6532 | 0.000 | 3 |
CeMnSbO (mp-542723) | 0.6108 | 0.108 | 4 |
CuBiTeO (mp-545369) | 0.6120 | 0.023 | 4 |
CeCdAsO (mp-10316) | 0.6212 | 0.045 | 4 |
CeZnSbO (mp-909296) | 0.6042 | 0.022 | 4 |
CeZnSbO (mp-22620) | 0.6065 | 0.022 | 4 |
Sn4Pt (mp-20662) | 0.6496 | 0.000 | 2 |
Sn4Au (mp-1393) | 0.6200 | 0.000 | 2 |
UTe3 (mp-8357) | 0.6428 | 0.042 | 2 |
HfTe3 (mp-1025459) | 0.6590 | 0.027 | 2 |
UTe3 (mp-568948) | 0.6513 | 0.042 | 2 |
Nd5Fe5As5O4F (mp-698941) | 0.6592 | 0.161 | 5 |
Ce8Fe8As8O7F (mp-705511) | 0.6297 | 0.099 | 5 |
SrNd7Fe8(AsO)8 (mp-705458) | 0.6636 | 0.208 | 5 |
Sm6Fe6As6O5F (mp-697821) | 0.5994 | 0.170 | 5 |
SrNd5Fe6(AsO)6 (mp-694989) | 0.6914 | 0.154 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: U Te P O |
Final Energy/Atom-7.9200 eV |
Corrected Energy-98.1024 eV
Uncorrected energy = -95.0404 eV
Composition-based energy adjustment (-0.687 eV/atom x 2.0 atoms) = -1.3740 eV
Composition-based energy adjustment (-0.422 eV/atom x 4.0 atoms) = -1.6880 eV
Corrected energy = -98.1024 eV
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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)