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-0.382 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.002 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. |
Density5.13 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToAg3AsS3 |
Band Gap1.494 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 MauguinR3c [161] |
HallR 3 2"c |
Point Group3m |
Crystal Systemtrigonal |
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 100.4 |
LaAlO3 (mp-2920) | <1 0 0> | <1 0 1> | 143.9 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 0> | 206.3 |
YVO4 (mp-19133) | <1 0 1> | <1 0 0> | 206.3 |
CdTe (mp-406) | <1 0 0> | <1 1 0> | 178.7 |
LaF3 (mp-905) | <1 0 1> | <1 0 0> | 206.3 |
TbScO3 (mp-31119) | <0 1 1> | <1 0 0> | 103.2 |
NdGaO3 (mp-3196) | <0 1 1> | <1 0 0> | 103.2 |
NdGaO3 (mp-3196) | <1 1 1> | <1 0 0> | 206.3 |
C (mp-48) | <0 0 1> | <0 0 1> | 100.4 |
SiC (mp-8062) | <1 1 1> | <0 0 1> | 100.4 |
TiO2 (mp-390) | <1 1 0> | <1 0 0> | 103.2 |
ZnO (mp-2133) | <1 0 0> | <1 0 0> | 103.2 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 103.2 |
CdS (mp-672) | <1 0 0> | <1 0 1> | 143.9 |
Te2W (mp-22693) | <0 0 1> | <0 0 1> | 200.7 |
MoS2 (mp-1434) | <1 0 0> | <1 0 0> | 206.3 |
TiO2 (mp-2657) | <1 0 1> | <1 0 0> | 103.2 |
TbScO3 (mp-31119) | <1 1 1> | <1 0 0> | 206.3 |
InSb (mp-20012) | <1 0 0> | <1 1 0> | 178.7 |
YAlO3 (mp-3792) | <0 1 1> | <0 0 1> | 100.4 |
TiO2 (mp-390) | <1 0 1> | <0 0 1> | 200.7 |
SrTiO3 (mp-4651) | <1 1 1> | <1 0 0> | 206.3 |
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 |
---|---|---|---|
Hg3(SF)2 (mp-7580) | 0.7201 | 0.000 | 3 |
Ag3AsSe3 (mp-5145) | 0.4389 | 0.012 | 3 |
CaCoN2 (mvc-11274) | 0.7079 | 0.627 | 3 |
ZnSnO2 (mvc-2430) | 0.6982 | 0.199 | 3 |
Ag3SbS3 (mp-4515) | 0.2741 | 0.001 | 3 |
GaSe (mp-568128) | 0.6352 | 0.399 | 2 |
InSe (mp-22691) | 0.6926 | 0.003 | 2 |
LiP5 (mp-2412) | 0.6608 | 0.013 | 2 |
InSe (mp-1079260) | 0.6967 | 0.000 | 2 |
InSe (mp-20485) | 0.6754 | 0.003 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ag As S |
Final Energy/Atom-3.7502 eV |
Corrected Energy-56.4835 eV
-56.4835 eV = -52.5028 eV (uncorrected energy) - 3.9808 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)