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-3.186 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. |
Density3.99 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToBaBPO5 + Ba2P2O7 |
Band Gap5.012 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 MauguinIbca [73] |
Hall-I 2b 2c |
Point Groupmmm |
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] |
---|---|---|---|
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 208.3 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 208.3 |
CdS (mp-672) | <1 1 1> | <0 0 1> | 104.2 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 208.3 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 104.2 |
YVO4 (mp-19133) | <1 0 1> | <0 0 1> | 208.3 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 208.3 |
Al (mp-134) | <1 1 0> | <0 0 1> | 208.3 |
Ni (mp-23) | <1 1 0> | <0 0 1> | 104.2 |
LaF3 (mp-905) | <1 0 0> | <0 0 1> | 104.2 |
BaTiO3 (mp-5986) | <0 0 1> | <0 0 1> | 208.3 |
Ni (mp-23) | <1 0 0> | <0 0 1> | 208.3 |
Cu (mp-30) | <1 0 0> | <0 0 1> | 104.2 |
LiAlO2 (mp-3427) | <1 1 1> | <0 0 1> | 104.2 |
LiAlO2 (mp-3427) | <0 0 1> | <0 1 0> | 162.8 |
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 |
---|---|---|---|
Ce2Si2O7 (mp-662527) | 0.4765 | 0.000 | 3 |
Ba2Si3O8 (mp-553897) | 0.5576 | 0.001 | 3 |
Rb2Cr2O7 (mp-616734) | 0.5145 | 0.000 | 3 |
Nd2Si2O7 (mp-556771) | 0.5296 | 0.003 | 3 |
Ba2Si3O8 (mp-29222) | 0.5497 | 0.000 | 3 |
NaEuP2O7 (mp-6272) | 0.4921 | 0.000 | 4 |
K2Nd(PO3)5 (mp-559732) | 0.4766 | 0.007 | 4 |
K2CrSO7 (mp-565687) | 0.4928 | 0.000 | 4 |
Rb3B(SO4)3 (mp-1020716) | 0.3941 | 0.000 | 4 |
K3B(SO4)3 (mp-1019789) | 0.3620 | 0.000 | 4 |
SrZnP2(HO4)2 (mp-697018) | 0.6525 | 0.851 | 5 |
TlZnSClO4 (mp-23146) | 0.5446 | 0.000 | 5 |
RbZnSClO4 (mp-559540) | 0.5391 | 0.000 | 5 |
GdP4H4NO12 (mp-560412) | 0.6099 | 0.005 | 5 |
RbPrP3HO10 (mp-601292) | 0.6306 | 0.035 | 5 |
NaZnP2HClO7 (mp-738635) | 0.6887 | 0.211 | 6 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv B P O |
Final Energy/Atom-7.3770 eV |
Corrected Energy-594.3599 eV
-594.3599 eV = -560.6500 eV (uncorrected energy) - 33.7099 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)