Final Magnetic Moment0.948 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-2.423 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.072 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. |
Density3.27 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToSnP2O7 + SnP4O11 |
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 MauguinP212121 [19] |
HallP 2ac 2ab |
Point Group222 |
Crystal Systemorthorhombic |
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] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 1 0> | <1 0 0> | 246.4 |
LaAlO3 (mp-2920) | <1 1 1> | <1 0 0> | 246.4 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 154.5 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 309.0 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 77.2 |
BaF2 (mp-1029) | <1 1 0> | <1 0 1> | 112.8 |
SiO2 (mp-6930) | <1 1 0> | <1 0 0> | 246.4 |
KCl (mp-23193) | <1 1 0> | <1 0 1> | 112.8 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 309.0 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 77.2 |
InAs (mp-20305) | <1 1 0> | <1 0 0> | 164.3 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 246.4 |
TePb (mp-19717) | <1 1 0> | <1 0 0> | 246.4 |
Te2Mo (mp-602) | <0 0 1> | <1 1 0> | 232.3 |
Ag (mp-124) | <1 0 0> | <0 0 1> | 154.5 |
Ag (mp-124) | <1 1 0> | <1 0 0> | 246.4 |
LiTaO3 (mp-3666) | <0 0 1> | <0 0 1> | 231.7 |
LiTaO3 (mp-3666) | <1 1 0> | <1 0 0> | 246.4 |
Fe3O4 (mp-19306) | <1 0 0> | <0 0 1> | 77.2 |
C (mp-66) | <1 1 0> | <1 0 0> | 164.3 |
LiNbO3 (mp-3731) | <0 0 1> | <0 0 1> | 231.7 |
LiNbO3 (mp-3731) | <1 1 0> | <1 0 0> | 246.4 |
LiNbO3 (mp-3731) | <1 1 1> | <1 0 0> | 246.4 |
LaF3 (mp-905) | <0 0 1> | <0 0 1> | 231.7 |
GaP (mp-2490) | <1 0 0> | <0 0 1> | 154.5 |
LiGaO2 (mp-5854) | <1 0 0> | <1 1 1> | 139.5 |
CdTe (mp-406) | <1 1 0> | <1 0 0> | 246.4 |
PbSe (mp-2201) | <1 0 0> | <0 0 1> | 77.2 |
PbSe (mp-2201) | <1 1 0> | <1 0 1> | 112.8 |
NdGaO3 (mp-3196) | <1 1 0> | <0 0 1> | 309.0 |
LiTaO3 (mp-3666) | <1 1 1> | <1 0 0> | 246.4 |
MgO (mp-1265) | <1 0 0> | <0 0 1> | 309.0 |
TiO2 (mp-2657) | <1 0 0> | <1 0 0> | 82.1 |
TiO2 (mp-2657) | <1 1 1> | <0 0 1> | 231.7 |
SiC (mp-11714) | <1 0 1> | <1 0 1> | 225.5 |
GdScO3 (mp-5690) | <1 1 0> | <0 0 1> | 309.0 |
CdSe (mp-2691) | <1 0 0> | <0 0 1> | 77.2 |
CdSe (mp-2691) | <1 1 0> | <1 0 0> | 164.3 |
InP (mp-20351) | <1 0 0> | <0 0 1> | 309.0 |
TbScO3 (mp-31119) | <1 1 0> | <0 0 1> | 309.0 |
Ni (mp-23) | <1 0 0> | <0 0 1> | 309.0 |
InSb (mp-20012) | <1 1 0> | <1 0 0> | 246.4 |
SiC (mp-8062) | <1 0 0> | <0 0 1> | 77.2 |
Ga2O3 (mp-886) | <1 0 -1> | <1 1 0> | 116.1 |
Ga2O3 (mp-886) | <1 0 0> | <1 0 0> | 164.3 |
Si (mp-149) | <1 0 0> | <0 0 1> | 154.5 |
Au (mp-81) | <1 0 0> | <0 0 1> | 154.5 |
Au (mp-81) | <1 1 0> | <1 0 1> | 225.5 |
CdWO4 (mp-19387) | <0 0 1> | <1 0 0> | 246.4 |
CsI (mp-614603) | <1 0 0> | <0 0 1> | 309.0 |
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 |
---|---|---|---|
Ni(PO3)3 (mp-767813) | 0.2766 | 0.025 | 3 |
V(PO3)3 (mp-767740) | 0.2657 | 0.050 | 3 |
Ni(PO3)3 (mp-850474) | 0.3394 | 0.014 | 3 |
MoP2O7 (mp-32065) | 0.3285 | 0.086 | 3 |
Cu(PO3)3 (mp-540496) | 0.3218 | 0.012 | 3 |
MnV(P2O7)2 (mp-774043) | 0.3652 | 0.006 | 4 |
LiSb(PO3)4 (mp-504340) | 0.3637 | 0.042 | 4 |
LiSn2P5O16 (mp-757964) | 0.3668 | 0.100 | 4 |
LiSn(PO3)4 (mp-757616) | 0.4121 | 0.078 | 4 |
LiSn3(P3O10)2 (mp-765222) | 0.3529 | 0.080 | 4 |
Cr3O8 (mp-782705) | 0.7218 | 0.115 | 2 |
V5O12 (mp-776915) | 0.7093 | 0.032 | 2 |
As2O5 (mp-555434) | 0.7334 | 0.004 | 2 |
Cr3O8 (mp-715515) | 0.7357 | 0.180 | 2 |
As2O5 (mp-1788) | 0.7239 | 0.000 | 2 |
MgCr3Se2(SO6)4 (mp-769544) | 0.5605 | 0.126 | 5 |
MgCr3Se3(SO8)3 (mp-773999) | 0.5726 | 0.180 | 5 |
LiBS4(ClO3)4 (mp-555090) | 0.6181 | 0.005 | 5 |
Cs3Mg3In(PO3)12 (mp-720658) | 0.5700 | 0.006 | 5 |
LiS2N(O2F)2 (mp-559971) | 0.6279 | 0.089 | 5 |
K3Na3TeP6(HO4)6 (mp-720804) | 0.5597 | 0.030 | 6 |
CsAlBP2HO9 (mp-542129) | 0.6106 | 0.000 | 6 |
RbAlBP2HO9 (mp-542130) | 0.6391 | 0.000 | 6 |
RbGaBP2HO9 (mp-24761) | 0.6758 | 0.000 | 6 |
CsFeBP2HO9 (mp-761395) | 0.6172 | 0.118 | 6 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Sn_d P O |
Final Energy/Atom-6.9191 eV |
Corrected Energy-384.5259 eV
Uncorrected energy = -359.7939 eV
Composition-based energy adjustment (-0.687 eV/atom x 36.0 atoms) = -24.7320 eV
Corrected energy = -384.5259 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)