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-0.688 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.132 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. |
Density4.38 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCa2SnN2 |
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 MauguinC2 [5] |
HallC 2y |
Point Group2 |
Crystal Systemmonoclinic |
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] |
---|---|---|---|
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 163.0 |
BaF2 (mp-1029) | <1 1 0> | <1 0 1> | 221.7 |
GaN (mp-804) | <1 0 0> | <1 0 -1> | 263.2 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 170.6 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 54.3 |
SiO2 (mp-6930) | <1 1 1> | <1 1 1> | 100.8 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 273.0 |
InAs (mp-20305) | <1 1 0> | <1 0 1> | 221.7 |
ZnSe (mp-1190) | <1 0 0> | <0 1 1> | 262.5 |
KTaO3 (mp-3614) | <1 0 0> | <0 1 1> | 262.5 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 204.7 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 271.7 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 170.6 |
CdS (mp-672) | <1 1 0> | <0 1 0> | 205.8 |
AlN (mp-661) | <0 0 1> | <0 1 1> | 262.5 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 108.7 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 54.3 |
GaAs (mp-2534) | <1 0 0> | <0 1 1> | 262.5 |
LiF (mp-1138) | <1 0 0> | <0 1 1> | 262.5 |
LiF (mp-1138) | <1 1 0> | <1 0 -1> | 210.6 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 170.6 |
Te2W (mp-22693) | <1 1 0> | <1 0 1> | 221.7 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 170.6 |
GaN (mp-804) | <1 0 1> | <0 1 1> | 262.5 |
GaN (mp-804) | <1 1 0> | <1 0 0> | 307.1 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 307.1 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 326.0 |
TePb (mp-19717) | <1 0 0> | <1 0 1> | 221.7 |
Te2Mo (mp-602) | <0 0 1> | <1 0 -1> | 263.2 |
KCl (mp-23193) | <1 0 0> | <0 1 0> | 205.8 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 0> | 307.1 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 -1> | 210.6 |
Ag (mp-124) | <1 1 1> | <1 0 1> | 147.8 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 102.4 |
GaSe (mp-1943) | <1 1 0> | <1 0 0> | 238.8 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 68.2 |
CdS (mp-672) | <1 1 1> | <0 1 0> | 205.8 |
LiF (mp-1138) | <1 1 1> | <1 0 1> | 147.8 |
BN (mp-984) | <0 0 1> | <1 0 0> | 238.8 |
BN (mp-984) | <1 0 0> | <1 0 -1> | 157.9 |
BN (mp-984) | <1 1 0> | <1 1 0> | 306.5 |
BN (mp-984) | <1 1 1> | <1 1 -1> | 173.0 |
Te2W (mp-22693) | <0 1 0> | <1 0 0> | 102.4 |
Te2W (mp-22693) | <1 1 1> | <1 1 0> | 229.9 |
YVO4 (mp-19133) | <1 0 0> | <1 1 0> | 229.9 |
YVO4 (mp-19133) | <1 1 0> | <1 1 -1> | 259.4 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 0 0> | 238.8 |
Ag (mp-124) | <1 0 0> | <1 0 1> | 221.7 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 217.3 |
Al (mp-134) | <1 1 1> | <1 0 0> | 204.7 |
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 |
---|---|---|---|
Mg2VN2 (mvc-15572) | 0.4253 | 0.170 | 3 |
Mg2WN2 (mvc-15551) | 0.3224 | 0.204 | 3 |
Mg2TiN2 (mvc-14558) | 0.3681 | 0.189 | 3 |
Na4PtO4 (mp-675073) | 0.5341 | 0.115 | 3 |
InBiS3 (mp-1078776) | 0.5402 | 0.003 | 3 |
Li3MnV3O8 (mp-868354) | 0.5527 | 0.091 | 4 |
LiFe(CoO3)2 (mp-763429) | 0.5878 | 0.060 | 4 |
LiCo2CuO6 (mp-763314) | 0.5624 | 0.112 | 4 |
LiMn2NiO6 (mp-762633) | 0.5321 | 0.080 | 4 |
LiCo2NiO6 (mp-774305) | 0.5464 | 0.036 | 4 |
Sc29S42 (mp-684978) | 0.7373 | 0.231 | 2 |
In6S7 (mp-555853) | 0.7176 | 0.008 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ca_sv Sn_d N |
Final Energy/Atom-5.4675 eV |
Corrected Energy-54.6752 eV
-54.6752 eV = -54.6752 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)