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-0.907 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.001 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. |
Density3.48 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToKSb5S8 + KSbS2 |
Band Gap1.553 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 |
Topological Classificationtrivial*
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SubclassificationLCEBR†
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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] |
---|---|---|---|
DyScO3 (mp-31120) | <0 1 0> | <1 0 1> | 172.2 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 254.3 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 -1> | 161.5 |
C (mp-66) | <1 0 0> | <0 0 1> | 254.3 |
MgO (mp-1265) | <1 1 1> | <0 0 1> | 254.3 |
GdScO3 (mp-5690) | <1 1 0> | <0 0 1> | 254.3 |
TbScO3 (mp-31119) | <0 1 0> | <1 0 1> | 172.2 |
TbScO3 (mp-31119) | <1 1 0> | <0 0 1> | 254.3 |
BaTiO3 (mp-5986) | <0 0 1> | <1 0 -1> | 161.5 |
NdGaO3 (mp-3196) | <1 1 0> | <0 0 1> | 254.3 |
NaCl (mp-22862) | <1 0 0> | <0 0 1> | 254.3 |
ZrO2 (mp-2858) | <1 0 1> | <0 0 1> | 84.8 |
CdWO4 (mp-19387) | <1 0 0> | <0 0 1> | 254.3 |
CsI (mp-614603) | <1 0 0> | <0 0 1> | 254.3 |
SrTiO3 (mp-4651) | <0 0 1> | <0 0 1> | 254.3 |
SrTiO3 (mp-4651) | <1 1 0> | <0 0 1> | 254.3 |
SrTiO3 (mp-4651) | <1 1 1> | <1 0 0> | 143.8 |
Ge (mp-32) | <1 1 0> | <1 0 0> | 143.8 |
LiAlO2 (mp-3427) | <1 0 1> | <0 0 1> | 84.8 |
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
CuClO2 (mp-997104) | 0.5730 | 0.291 | 3 |
TlSb3S5 (mp-27515) | 0.4101 | 0.004 | 3 |
Rb2Bi4O7 (mp-556735) | 0.5664 | 0.000 | 3 |
Cs(SbSe2)2 (mp-3312) | 0.5347 | 0.000 | 3 |
Cs(SbS2)2 (mp-8890) | 0.4828 | 0.000 | 3 |
LiVOF3 (mp-765498) | 0.6742 | 0.071 | 4 |
Rb3Ta2AgSe12 (mp-569378) | 0.7265 | 0.000 | 4 |
TeO2 (mp-8377) | 0.7371 | 0.011 | 2 |
Al4C3 (mp-743752) | 0.5470 | 0.585 | 2 |
Bi2O3 (mp-556549) | 0.7316 | 0.024 | 2 |
TeO2 (mp-2125) | 0.6968 | 0.000 | 2 |
Sb2O3 (mp-2136) | 0.6819 | 0.000 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: K_sv Sb S |
Final Energy/Atom-4.2186 eV |
Corrected Energy-116.7259 eV
Uncorrected energy = -109.6839 eV
Composition-based energy adjustment (-0.503 eV/atom x 14.0 atoms) = -7.0420 eV
Corrected energy = -116.7259 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)