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-2.183 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.049 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. |
Density6.78 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToDy2S3 + PbS |
Band Gap2.130 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 [5] |
HallC 2y |
Point Group2 |
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] |
---|---|---|---|
LiF (mp-1138) | <1 0 0> | <0 0 1> | 100.3 |
TeO2 (mp-2125) | <0 1 0> | <0 0 1> | 200.7 |
TeO2 (mp-2125) | <1 0 0> | <0 0 1> | 200.7 |
Fe3O4 (mp-19306) | <1 1 0> | <0 0 1> | 100.3 |
MgO (mp-1265) | <1 1 0> | <0 0 1> | 100.3 |
C (mp-66) | <1 1 0> | <0 0 1> | 200.7 |
PbS (mp-21276) | <1 1 0> | <0 0 1> | 100.3 |
InP (mp-20351) | <1 1 0> | <0 0 1> | 100.3 |
BaTiO3 (mp-5986) | <1 0 0> | <0 0 1> | 100.3 |
Cu (mp-30) | <1 1 0> | <0 0 1> | 200.7 |
Au (mp-81) | <1 1 0> | <0 0 1> | 100.3 |
MgAl2O4 (mp-3536) | <1 0 0> | <0 0 1> | 200.7 |
GaTe (mp-542812) | <1 0 -1> | <1 0 0> | 158.3 |
Al2O3 (mp-1143) | <0 0 1> | <1 0 0> | 158.3 |
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 |
---|---|---|---|
Tb14(PbSe8)3 (mp-676110) | 0.1587 | 0.043 | 3 |
Ho14(PbS8)3 (mp-675425) | 0.1044 | 0.059 | 3 |
Tb6CdS10 (mp-530870) | 0.3112 | 0.046 | 3 |
La6YbSe10 (mp-530910) | 0.3505 | 0.000 | 3 |
Tb6PbSe10 (mp-675130) | 0.2655 | 0.040 | 3 |
Ho2Se3 (mp-685041) | 0.3345 | 0.064 | 2 |
Sm39S56 (mp-684860) | 0.3345 | 0.024 | 2 |
Lu2Se3 (mp-673650) | 0.3215 | 0.110 | 2 |
Er2Se3 (mp-32736) | 0.3192 | 0.076 | 2 |
Tm2Se3 (mp-32850) | 0.3185 | 0.087 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Dy_3 Pb_d S |
Final Energy/Atom-6.0610 eV |
Corrected Energy-264.4242 eV
-264.4242 eV = -248.5012 eV (uncorrected energy) - 15.9230 eV (MP Anion Correction)
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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)