Final Magnetic Moment0.731 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-0.105 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.738 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. |
Density4.65 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToScCoSi |
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 MauguinCmcm [63] |
Hall-C 2c 2 |
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%)
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
C (mp-48) | <0 0 1> | <0 1 0> | 64.6 |
C (mp-48) | <1 0 1> | <0 1 0> | 167.9 |
C (mp-48) | <1 1 0> | <0 1 0> | 271.2 |
C (mp-48) | <1 0 0> | <0 1 0> | 38.7 |
C (mp-48) | <1 1 1> | <0 1 0> | 271.2 |
LaAlO3 (mp-2920) | <0 0 1> | <0 1 0> | 348.7 |
AlN (mp-661) | <1 0 1> | <0 1 0> | 193.7 |
AlN (mp-661) | <1 1 0> | <0 1 0> | 219.5 |
AlN (mp-661) | <1 1 1> | <0 1 0> | 116.2 |
AlN (mp-661) | <0 0 1> | <0 1 0> | 245.4 |
AlN (mp-661) | <1 0 0> | <0 1 0> | 77.5 |
CeO2 (mp-20194) | <1 0 0> | <0 1 0> | 116.2 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 161.1 |
GaAs (mp-2534) | <1 0 0> | <0 1 0> | 64.6 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 322.8 |
BaF2 (mp-1029) | <1 0 0> | <0 1 0> | 206.6 |
BaF2 (mp-1029) | <1 1 0> | <1 0 1> | 222.8 |
BaF2 (mp-1029) | <1 1 1> | <1 1 0> | 268.5 |
SiO2 (mp-6930) | <1 0 0> | <0 1 0> | 219.5 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 245.4 |
SiO2 (mp-6930) | <1 1 0> | <0 1 0> | 193.7 |
SiO2 (mp-6930) | <0 0 1> | <0 1 0> | 64.6 |
KCl (mp-23193) | <1 0 0> | <0 1 0> | 167.9 |
KCl (mp-23193) | <1 1 0> | <1 0 1> | 222.8 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 284.1 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 0> | 322.8 |
DyScO3 (mp-31120) | <1 0 1> | <1 1 1> | 226.1 |
DyScO3 (mp-31120) | <1 1 0> | <0 1 0> | 64.6 |
DyScO3 (mp-31120) | <0 1 0> | <0 1 0> | 129.1 |
DyScO3 (mp-31120) | <0 1 1> | <0 1 0> | 219.5 |
InAs (mp-20305) | <1 0 0> | <0 1 0> | 322.8 |
InAs (mp-20305) | <1 1 1> | <1 1 0> | 268.5 |
InAs (mp-20305) | <1 1 0> | <1 0 1> | 222.8 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 322.8 |
KTaO3 (mp-3614) | <1 1 1> | <0 1 0> | 206.6 |
ZnSe (mp-1190) | <1 0 0> | <0 1 0> | 64.6 |
KTaO3 (mp-3614) | <1 0 0> | <0 1 0> | 64.6 |
KTaO3 (mp-3614) | <1 1 0> | <0 1 0> | 206.6 |
InP (mp-20351) | <1 0 0> | <0 1 0> | 322.8 |
InP (mp-20351) | <1 1 0> | <1 0 1> | 148.5 |
InP (mp-20351) | <1 1 1> | <0 1 0> | 309.9 |
Te2W (mp-22693) | <0 1 0> | <1 1 0> | 53.7 |
Te2W (mp-22693) | <0 1 1> | <0 1 0> | 116.2 |
CdWO4 (mp-19387) | <1 0 0> | <1 1 1> | 150.7 |
Te2W (mp-22693) | <0 0 1> | <0 1 0> | 90.4 |
Te2W (mp-22693) | <1 0 0> | <1 1 1> | 301.5 |
Te2W (mp-22693) | <1 1 0> | <1 1 0> | 107.4 |
CdWO4 (mp-19387) | <1 0 1> | <0 1 0> | 129.1 |
CdWO4 (mp-19387) | <1 1 0> | <0 1 0> | 129.1 |
CdWO4 (mp-19387) | <0 0 1> | <1 0 1> | 148.5 |
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.
Once you have registered you can also "vote" for full calculation of this material's elastic properties.
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
TmSnGe (mp-1025129) | 0.3430 | 0.000 | 3 |
ErSnGe (mp-1071492) | 0.4052 | 0.000 | 3 |
HoSnGe (mp-1077485) | 0.3307 | 0.000 | 3 |
TbSnGe (mp-1077556) | 0.2311 | 0.000 | 3 |
DySnGe (mp-1080405) | 0.2652 | 0.000 | 3 |
LuGe2 (mp-973906) | 0.3866 | 0.000 | 2 |
ThGe2 (mp-16372) | 0.4954 | 0.033 | 2 |
ZrSi2 (mp-1515) | 0.4447 | 0.000 | 2 |
TmGe2 (mp-13037) | 0.3595 | 0.000 | 2 |
HfSi2 (mp-1069) | 0.4604 | 0.000 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Sc_sv Co Si |
Final Energy/Atom-6.3937 eV |
Corrected Energy-38.3623 eV
-38.3623 eV = -38.3623 eV (uncorrected energy)
|
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)