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-1.193 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. |
Density3.80 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.969 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 MauguinC2/c [15] |
Hall-C 2yc |
Point Group2/m |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 167.6 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 167.6 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 167.6 |
Al (mp-134) | <1 1 1> | <0 0 1> | 167.6 |
CaCO3 (mp-3953) | <1 0 0> | <0 0 1> | 167.6 |
GdScO3 (mp-5690) | <0 1 1> | <0 0 1> | 167.6 |
GdScO3 (mp-5690) | <1 0 1> | <0 0 1> | 167.6 |
TbScO3 (mp-31119) | <1 0 1> | <0 0 1> | 167.6 |
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Cs4Tc6S13 (mp-579058) | 0.3168 | 0.000 | 3 |
Rb4Re6S13 (mp-541057) | 0.2330 | 0.000 | 3 |
K2(TcS2)3 (mp-541353) | 0.5161 | 0.000 | 3 |
K2(ReS2)3 (mp-541638) | 0.4979 | 0.000 | 3 |
Cs4Re6S13 (mp-652494) | 0.3935 | 0.000 | 3 |
TlRe6Se8Cl3 (mp-23635) | 0.7112 | 0.000 | 4 |
K2Rb2Re6S13 (mp-650124) | 0.4090 | 0.003 | 4 |
CsRe6Se8I3 (mp-680185) | 0.6351 | 0.000 | 4 |
TlRe3(Se2Cl)2 (mp-23144) | 0.6532 | 0.001 | 4 |
CsRe6S8Br3 (mp-669564) | 0.6140 | 0.006 | 4 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Rb_sv Tc_pv S |
Final Energy/Atom-6.0294 eV |
Corrected Energy-290.4297 eV
Uncorrected energy = -277.3517 eV
Composition-based energy adjustment (-0.503 eV/atom x 26.0 atoms) = -13.0780 eV
Corrected energy = -290.4297 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)