Final Magnetic Moment1.000 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-2.257 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.089 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. |
Density3.56 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToSn3(PO4)2 + SnP2O7 + SnO2 |
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 MauguinR3c [161] |
HallR 3 2"c |
Point Group3m |
Crystal Systemtrigonal |
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] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <0 0 1> | 250.7 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 83.6 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 250.7 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 167.1 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 250.7 |
Al (mp-134) | <1 1 1> | <0 0 1> | 83.6 |
C (mp-66) | <1 1 0> | <0 0 1> | 250.7 |
GdScO3 (mp-5690) | <0 1 1> | <0 0 1> | 167.1 |
GdScO3 (mp-5690) | <1 0 1> | <0 0 1> | 167.1 |
PbS (mp-21276) | <1 1 1> | <0 0 1> | 250.7 |
InP (mp-20351) | <1 1 1> | <0 0 1> | 250.7 |
TbScO3 (mp-31119) | <1 0 1> | <0 0 1> | 167.1 |
Ni (mp-23) | <1 1 1> | <0 0 1> | 83.6 |
NdGaO3 (mp-3196) | <1 0 1> | <0 0 1> | 167.1 |
ZnO (mp-2133) | <0 0 1> | <0 0 1> | 83.6 |
SrTiO3 (mp-4651) | <1 0 1> | <0 0 1> | 167.1 |
Al2O3 (mp-1143) | <1 0 0> | <0 0 1> | 250.7 |
ZnTe (mp-2176) | <1 1 1> | <0 0 1> | 250.7 |
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 |
---|---|---|---|
AsPO4 (mp-8140) | 0.6821 | 0.000 | 3 |
Tl8Ge5O14 (mp-27271) | 0.6697 | 0.000 | 3 |
Sn3(PO4)2 (mp-27493) | 0.4920 | 0.000 | 3 |
Si3Sb2O9 (mp-769028) | 0.7019 | 0.010 | 3 |
Sn2P2O7 (mp-554022) | 0.5758 | 0.000 | 3 |
As2PHO6 (mp-707231) | 0.7395 | 0.042 | 4 |
KSn4(PO4)3 (mp-6755) | 0.6679 | 0.000 | 4 |
SnPO3F (mp-555838) | 0.6802 | 0.000 | 4 |
LiSn4(PO4)3 (mp-765150) | 0.7162 | 0.079 | 4 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Sn_d P O |
Final Energy/Atom-6.6333 eV |
Corrected Energy-268.9191 eV
-268.9191 eV = -252.0642 eV (uncorrected energy) - 16.8550 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)