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 / Atom0.006 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.006 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. |
Density1.74 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToC |
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 MauguinP63/mmc [194] |
Hall-P 6c 2c |
Point Group6/mmm |
Crystal Systemhexagonal |
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%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
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substrate material | substrate orientation | film orientation | elastic energy [meV] | MCIA† [Å2] |
---|---|---|---|---|
Fe2O3 (mp-24972) | <0 0 1> | <0 0 1> | 0.001 | 68.5 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 0.001 | 68.5 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 0.001 | 84.4 |
CsI (mp-614603) | <1 1 0> | <1 0 0> | 0.004 | 173.3 |
LiAlO2 (mp-3427) | <1 1 0> | <1 0 0> | 0.006 | 231.0 |
BaF2 (mp-1029) | <1 1 1> | <0 0 1> | 0.009 | 68.5 |
TbScO3 (mp-31119) | <0 1 1> | <1 0 1> | 0.010 | 159.7 |
ZnO (mp-2133) | <1 0 0> | <1 0 0> | 0.010 | 154.0 |
CdWO4 (mp-19387) | <1 0 1> | <1 0 0> | 0.022 | 173.3 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 1> | 0.026 | 159.7 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 0.033 | 226.7 |
Al (mp-134) | <1 1 1> | <0 0 1> | 0.041 | 84.4 |
GdScO3 (mp-5690) | <0 1 1> | <1 0 1> | 0.043 | 159.7 |
SiC (mp-8062) | <1 1 1> | <0 0 1> | 0.043 | 100.2 |
Te2Mo (mp-602) | <1 0 0> | <0 0 1> | 0.046 | 274.1 |
Mg (mp-153) | <1 0 0> | <1 0 1> | 0.066 | 99.8 |
SiC (mp-7631) | <0 0 1> | <0 0 1> | 0.067 | 100.2 |
MgO (mp-1265) | <1 1 0> | <1 1 0> | 0.067 | 100.0 |
TeO2 (mp-2125) | <1 1 0> | <1 0 0> | 0.072 | 96.3 |
SiC (mp-11714) | <0 0 1> | <0 0 1> | 0.079 | 100.2 |
TePb (mp-19717) | <1 0 0> | <1 1 0> | 0.081 | 300.1 |
TeO2 (mp-2125) | <1 1 1> | <1 0 0> | 0.083 | 211.8 |
CdTe (mp-406) | <1 1 1> | <0 0 1> | 0.090 | 226.7 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 0.103 | 142.3 |
CaF2 (mp-2741) | <1 1 0> | <1 0 0> | 0.117 | 173.3 |
GdScO3 (mp-5690) | <0 1 0> | <1 0 0> | 0.120 | 173.3 |
Cu (mp-30) | <1 1 1> | <0 0 1> | 0.121 | 68.5 |
InSb (mp-20012) | <1 1 1> | <0 0 1> | 0.124 | 226.7 |
MgO (mp-1265) | <1 0 0> | <0 0 1> | 0.138 | 126.5 |
NaCl (mp-22862) | <1 0 0> | <0 0 1> | 0.146 | 258.3 |
LiF (mp-1138) | <1 1 0> | <1 1 1> | 0.152 | 168.8 |
CdWO4 (mp-19387) | <1 1 0> | <1 0 0> | 0.168 | 250.3 |
SiC (mp-7631) | <1 1 1> | <0 0 1> | 0.174 | 163.4 |
CdWO4 (mp-19387) | <0 1 1> | <1 1 1> | 0.178 | 202.6 |
NdGaO3 (mp-3196) | <0 0 1> | <0 0 1> | 0.184 | 184.5 |
GaP (mp-2490) | <1 1 0> | <1 0 0> | 0.190 | 173.3 |
Ni (mp-23) | <1 1 1> | <0 0 1> | 0.198 | 21.1 |
LiGaO2 (mp-5854) | <1 1 1> | <1 0 1> | 0.213 | 219.6 |
Si (mp-149) | <1 0 0> | <0 0 1> | 0.214 | 210.9 |
LiAlO2 (mp-3427) | <1 1 1> | <0 0 1> | 0.218 | 268.9 |
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 0.225 | 210.9 |
LiAlO2 (mp-3427) | <1 0 0> | <1 0 1> | 0.234 | 99.8 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 0.234 | 226.7 |
TeO2 (mp-2125) | <1 0 0> | <0 0 1> | 0.236 | 210.9 |
DyScO3 (mp-31120) | <1 0 0> | <1 1 0> | 0.237 | 133.4 |
Ga2O3 (mp-886) | <0 1 0> | <1 0 0> | 0.248 | 211.8 |
Cu (mp-30) | <1 0 0> | <1 0 0> | 0.254 | 173.3 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 0.275 | 100.2 |
ZrO2 (mp-2858) | <1 1 0> | <0 0 1> | 0.280 | 79.1 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 0.283 | 184.5 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
904 | 159 | -1 | 0 | 0 | 0 |
159 | 904 | -1 | 0 | 0 | 0 |
-1 | -1 | 8 | 0 | 0 | 0 |
0 | 0 | 0 | 2 | 0 | 0 |
0 | 0 | 0 | 0 | 2 | 0 |
0 | 0 | 0 | 0 | 0 | 372 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
1.1 | -0.2 | 0.1 | -0.0 | 0.0 | 0.0 |
-0.2 | 1.1 | 0.1 | -0.0 | 0.0 | 0.0 |
0.1 | 0.1 | 131.9 | -0.0 | 0.0 | 0.0 |
-0.0 | -0.0 | -0.0 | 404.7 | 0.0 | 0.0 |
0.0 | -0.0 | 0.0 | 0.0 | 404.7 | 0.0 |
0.0 | 0.0 | 0.0 | 0.0 | 0.0 | 2.7 |
Shear Modulus GV186 GPa |
Bulk Modulus KV236 GPa |
Shear Modulus GR5 GPa |
Bulk Modulus KR7 GPa |
Shear Modulus GVRH96 GPa |
Bulk Modulus KVRH122 GPa |
Elastic Anisotropy210.07 |
Poisson's Ratio0.19 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
B3C10N3 (mp-642462) | 0.1838 | 0.587 | 3 |
BN (mp-629015) | 0.1096 | 0.004 | 2 |
GaN (mp-1007824) | 0.1848 | 0.354 | 2 |
BN (mp-685145) | 0.1836 | 0.007 | 2 |
BN (mp-7991) | 0.0305 | 0.000 | 2 |
BN (mp-604884) | 0.1293 | 0.004 | 2 |
C (mp-568286) | 0.1142 | 0.006 | 1 |
C (mp-997182) | 0.1199 | 0.008 | 1 |
C (mp-990448) | 0.1267 | 0.008 | 1 |
C (mp-937760) | 0.1154 | 0.004 | 1 |
C (mp-1018088) | 0.1181 | 1.305 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: C |
Final Energy/Atom-9.2203 eV |
Corrected Energy-36.8812 eV
Uncorrected energy = -36.8812 eV
Corrected energy = -36.8812 eV
|
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)