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 / Atom0.075 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.684 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. |
Density2.84 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCaN2 + Ba(CoN)2 |
Band Gap0.250 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 MauguinPna21 [33] |
HallP 2c 2n |
Point Groupmm2 |
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] |
---|---|---|---|
AlN (mp-661) | <1 0 0> | <0 1 0> | 202.7 |
AlN (mp-661) | <1 1 1> | <0 1 0> | 202.7 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 260.1 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 65.0 |
GaAs (mp-2534) | <1 1 0> | <0 0 1> | 325.2 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 144.0 |
AlN (mp-661) | <1 1 0> | <0 1 1> | 240.8 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 325.2 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 325.2 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 65.0 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 325.2 |
GaN (mp-804) | <0 0 1> | <1 1 0> | 144.0 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 325.2 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 325.2 |
CdS (mp-672) | <1 0 0> | <0 0 1> | 325.2 |
YVO4 (mp-19133) | <0 0 1> | <0 0 1> | 260.1 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 130.1 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 325.2 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 65.0 |
ZnSe (mp-1190) | <1 1 0> | <0 0 1> | 325.2 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 65.0 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 325.2 |
CdS (mp-672) | <1 1 1> | <0 0 1> | 260.1 |
Ag (mp-124) | <1 1 0> | <0 0 1> | 195.1 |
BN (mp-984) | <1 0 0> | <0 0 1> | 195.1 |
BN (mp-984) | <1 0 1> | <0 0 1> | 260.1 |
BN (mp-984) | <1 1 1> | <0 1 1> | 240.8 |
LiF (mp-1138) | <1 0 0> | <0 1 0> | 101.3 |
LiF (mp-1138) | <1 1 0> | <0 0 1> | 325.2 |
YVO4 (mp-19133) | <1 1 1> | <0 1 1> | 240.8 |
LiGaO2 (mp-5854) | <1 0 1> | <0 0 1> | 130.1 |
TeO2 (mp-2125) | <0 1 1> | <1 1 1> | 158.0 |
TeO2 (mp-2125) | <1 0 0> | <1 1 0> | 144.0 |
LiNbO3 (mp-3731) | <1 0 1> | <0 1 1> | 240.8 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 325.2 |
Al (mp-134) | <1 0 0> | <0 0 1> | 65.0 |
Al (mp-134) | <1 1 0> | <0 0 1> | 325.2 |
SiC (mp-7631) | <0 0 1> | <0 0 1> | 325.2 |
TeO2 (mp-2125) | <1 1 0> | <0 1 0> | 101.3 |
C (mp-66) | <1 1 0> | <0 0 1> | 325.2 |
SiC (mp-7631) | <1 1 0> | <0 1 1> | 240.8 |
SiC (mp-7631) | <1 1 1> | <0 1 1> | 240.8 |
LiTaO3 (mp-3666) | <1 0 1> | <0 1 1> | 240.8 |
GdScO3 (mp-5690) | <0 1 0> | <0 0 1> | 130.1 |
GdScO3 (mp-5690) | <1 0 0> | <0 0 1> | 325.2 |
GdScO3 (mp-5690) | <1 0 1> | <0 0 1> | 325.2 |
Mg (mp-153) | <1 1 0> | <0 0 1> | 260.1 |
MgO (mp-1265) | <1 0 0> | <0 0 1> | 325.2 |
C (mp-66) | <1 0 0> | <0 0 1> | 65.0 |
GaP (mp-2490) | <1 1 0> | <0 0 1> | 130.1 |
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 |
---|---|---|---|
CaCoN2 (mvc-11274) | 0.5114 | 0.627 | 3 |
Hg2SeO3 (mp-30286) | 0.7371 | 0.006 | 3 |
LiAgF4 (mp-758054) | 0.7045 | 0.039 | 3 |
Na2SO3 (mp-35248) | 0.6907 | 0.604 | 3 |
LiAg(CO2)2 (mp-985572) | 0.7140 | 0.172 | 4 |
LiAg(CO2)2 (mp-985575) | 0.6542 | 0.173 | 4 |
LiB2SbO5 (mp-770808) | 0.7347 | 0.093 | 4 |
LiBSbO3 (mp-756853) | 0.6471 | 0.092 | 4 |
Cu5Se2(ClO4)2 (mp-554163) | 0.7190 | 0.010 | 4 |
ZnCuTeCl2O3 (mp-680388) | 0.6815 | 0.009 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ba_sv Ca_sv Co N |
Final Energy/Atom-6.1685 eV |
Corrected Energy-197.3928 eV
-197.3928 eV = -197.3928 eV (uncorrected energy)
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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)