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-0.573 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.000 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. |
Density7.47 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
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 MauguinP62m [189] |
HallP 6 2 |
Point Group6m2 |
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%)
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 0 0> | <1 0 0> | 276.1 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 313.2 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 306.8 |
AlN (mp-661) | <1 1 0> | <1 0 0> | 245.5 |
AlN (mp-661) | <1 1 1> | <1 0 0> | 276.1 |
CeO2 (mp-20194) | <1 1 0> | <1 0 1> | 162.7 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 178.9 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 337.5 |
GaN (mp-804) | <1 0 1> | <1 1 0> | 265.7 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 313.2 |
SiO2 (mp-6930) | <1 0 0> | <1 0 0> | 245.5 |
SiO2 (mp-6930) | <1 0 1> | <1 0 0> | 184.1 |
KCl (mp-23193) | <1 0 0> | <1 1 0> | 159.4 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 223.7 |
DyScO3 (mp-31120) | <1 1 1> | <1 0 0> | 276.1 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 184.1 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 223.7 |
KTaO3 (mp-3614) | <1 0 0> | <1 1 0> | 159.4 |
KTaO3 (mp-3614) | <1 1 0> | <1 1 0> | 212.6 |
CdS (mp-672) | <1 0 1> | <1 1 0> | 265.7 |
CdS (mp-672) | <1 1 0> | <1 0 0> | 245.5 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 212.6 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 223.7 |
Te2W (mp-22693) | <1 1 0> | <1 0 1> | 108.5 |
TePb (mp-19717) | <1 0 0> | <1 0 1> | 217.0 |
TePb (mp-19717) | <1 1 1> | <0 0 1> | 313.2 |
Te2Mo (mp-602) | <1 0 0> | <1 0 0> | 214.8 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 178.9 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 134.2 |
BaF2 (mp-1029) | <1 0 0> | <1 1 0> | 159.4 |
BaF2 (mp-1029) | <1 1 0> | <0 0 1> | 223.7 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 153.4 |
SiO2 (mp-6930) | <0 0 1> | <1 1 0> | 106.3 |
SiO2 (mp-6930) | <1 1 1> | <0 0 1> | 268.4 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 306.8 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 214.8 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 0> | 214.8 |
InAs (mp-20305) | <1 1 1> | <1 1 0> | 318.9 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 178.9 |
CdS (mp-672) | <0 0 1> | <1 0 0> | 30.7 |
CdS (mp-672) | <1 0 0> | <1 1 0> | 265.7 |
LiF (mp-1138) | <1 0 0> | <1 0 1> | 217.0 |
Te2W (mp-22693) | <0 0 1> | <1 0 0> | 92.0 |
Te2W (mp-22693) | <1 1 1> | <0 0 1> | 223.7 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 153.4 |
YVO4 (mp-19133) | <1 0 0> | <1 0 0> | 92.0 |
YVO4 (mp-19133) | <1 0 1> | <1 0 0> | 276.1 |
YVO4 (mp-19133) | <1 1 0> | <1 0 1> | 325.5 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 44.7 |
Te2Mo (mp-602) | <1 0 1> | <0 0 1> | 223.7 |
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 |
---|---|---|---|
GdAgGe (mp-9341) | 0.0412 | 0.000 | 3 |
DyAgGe (mp-567574) | 0.0427 | 0.000 | 3 |
GdSiAg (mp-1079690) | 0.0411 | 0.000 | 3 |
HfAsRu (mp-1079079) | 0.0576 | 0.000 | 3 |
HfPOs (mp-1080463) | 0.0484 | 0.000 | 3 |
Yb3In3Ge2Au (mp-981207) | 0.1153 | 0.000 | 4 |
LiYb2InGe2 (mp-977355) | 0.4816 | 0.000 | 4 |
Sr2LiInGe2 (mp-571617) | 0.5210 | 0.000 | 4 |
LiCa2InGe2 (mp-570850) | 0.4834 | 0.000 | 4 |
U3Al3NiRu2 (mp-1080528) | 0.3225 | 0.088 | 4 |
Fe2P (mp-778) | 0.1915 | 0.000 | 2 |
BaI2 (mp-568536) | 0.3402 | 0.006 | 2 |
BaCl2 (mp-567680) | 0.2807 | 0.030 | 2 |
Co2P (mp-13446) | 0.3743 | 0.022 | 2 |
Co2As (mp-1079254) | 0.2950 | 0.071 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Sm_3 Si Ag |
Final Energy/Atom-4.8985 eV |
Corrected Energy-44.0869 eV
-44.0869 eV = -44.0869 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)