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-1.496 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.111 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. |
Density2.27 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToHF + AsF3 + CS14 + C |
Band Gap2.792 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 MauguinP1 [2] |
Hall-P 1 |
Point Group1 |
Crystal Systemtriclinic |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <0 1 0> | 246.4 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 188.4 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 188.4 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 282.6 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 188.4 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 282.6 |
BN (mp-984) | <1 0 0> | <0 1 -1> | 250.0 |
LiGaO2 (mp-5854) | <1 1 1> | <0 0 1> | 282.6 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 -1> | 172.8 |
TeO2 (mp-2125) | <1 0 0> | <0 0 1> | 282.6 |
SiC (mp-7631) | <1 1 0> | <0 1 -1> | 250.0 |
LiGaO2 (mp-5854) | <0 0 1> | <0 1 -1> | 250.0 |
SiC (mp-7631) | <0 0 1> | <0 1 -1> | 125.0 |
SiC (mp-7631) | <1 1 1> | <0 1 0> | 246.4 |
Mg (mp-153) | <1 0 0> | <1 -1 1> | 199.9 |
PbS (mp-21276) | <1 0 0> | <0 0 1> | 282.6 |
InP (mp-20351) | <1 0 0> | <0 0 1> | 282.6 |
Ni (mp-23) | <1 0 0> | <0 0 1> | 282.6 |
Au (mp-81) | <1 0 0> | <0 0 1> | 282.6 |
SiC (mp-11714) | <0 0 1> | <0 1 -1> | 125.0 |
C (mp-48) | <1 0 0> | <0 1 -1> | 250.0 |
Ga2O3 (mp-886) | <0 1 0> | <0 0 1> | 282.6 |
ZrO2 (mp-2858) | <1 0 -1> | <0 0 1> | 282.6 |
ZrO2 (mp-2858) | <0 0 1> | <0 1 -1> | 250.0 |
ZrO2 (mp-2858) | <0 1 0> | <0 1 0> | 246.4 |
ZrO2 (mp-2858) | <1 0 0> | <1 0 -1> | 172.8 |
SiC (mp-8062) | <1 1 1> | <1 -1 1> | 199.9 |
YAlO3 (mp-3792) | <0 0 1> | <0 1 -1> | 250.0 |
CdWO4 (mp-19387) | <0 1 1> | <0 0 1> | 282.6 |
ZnO (mp-2133) | <1 0 1> | <0 0 1> | 282.6 |
Cu (mp-30) | <1 0 0> | <0 1 0> | 246.4 |
Al2O3 (mp-1143) | <0 0 1> | <0 0 1> | 282.6 |
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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Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: As H C S F |
Final Energy/Atom-4.5356 eV |
Corrected Energy-392.9297 eV
-392.9297 eV = -380.9874 eV (uncorrected energy) - 11.9423 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)