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-0.329 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. |
Density12.55 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 MauguinFm3m [225] |
Hall-F 4 2 3 |
Point Groupm3m |
Crystal Systemcubic |
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.
Apply Gaussian smoothing:
Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
AlN (mp-661) | <0 0 1> | <1 1 1> | 261.3 |
AlN (mp-661) | <1 0 0> | <1 0 0> | 251.4 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 251.4 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 251.4 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 142.2 |
BaF2 (mp-1029) | <1 1 0> | <1 1 0> | 213.4 |
BaF2 (mp-1029) | <1 1 1> | <1 1 1> | 261.3 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 284.5 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 0> | 213.4 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 251.4 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 201.2 |
InAs (mp-20305) | <1 1 1> | <1 1 1> | 261.3 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 142.2 |
ZnSe (mp-1190) | <1 1 1> | <1 1 0> | 284.5 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 251.4 |
CdS (mp-672) | <0 0 1> | <1 0 0> | 150.9 |
LiF (mp-1138) | <1 1 1> | <1 1 1> | 87.1 |
Te2W (mp-22693) | <0 0 1> | <1 1 0> | 284.5 |
Te2W (mp-22693) | <0 1 0> | <1 1 0> | 213.4 |
Ag (mp-124) | <1 1 1> | <1 0 0> | 150.9 |
BN (mp-984) | <1 0 0> | <1 0 0> | 150.9 |
BN (mp-984) | <1 1 0> | <1 1 1> | 261.3 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 0 0> | 150.9 |
Al (mp-134) | <1 1 0> | <1 1 0> | 71.1 |
Al (mp-134) | <1 1 1> | <1 1 1> | 87.1 |
LiGaO2 (mp-5854) | <0 1 0> | <1 0 0> | 251.4 |
Fe3O4 (mp-19306) | <1 1 0> | <1 1 0> | 213.4 |
MgO (mp-1265) | <1 1 0> | <1 1 0> | 284.5 |
TiO2 (mp-2657) | <1 0 1> | <1 1 0> | 284.5 |
C (mp-66) | <1 0 0> | <1 0 0> | 50.3 |
C (mp-66) | <1 1 0> | <1 1 0> | 71.1 |
C (mp-66) | <1 1 1> | <1 1 1> | 87.1 |
GdScO3 (mp-5690) | <0 1 1> | <1 1 0> | 284.5 |
GdScO3 (mp-5690) | <1 0 1> | <1 1 1> | 174.2 |
GdScO3 (mp-5690) | <1 1 0> | <1 0 0> | 251.4 |
KP(HO2)2 (mp-23959) | <0 0 1> | <1 0 0> | 150.9 |
KP(HO2)2 (mp-23959) | <0 1 1> | <1 1 0> | 213.4 |
TbScO3 (mp-31119) | <0 1 1> | <1 1 0> | 213.4 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 213.4 |
GaAs (mp-2534) | <1 1 1> | <1 1 0> | 284.5 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 201.2 |
SiO2 (mp-6930) | <0 0 1> | <1 1 1> | 87.1 |
SiO2 (mp-6930) | <1 1 1> | <1 1 0> | 213.4 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 201.2 |
InAs (mp-20305) | <1 1 0> | <1 1 0> | 213.4 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 251.4 |
CdS (mp-672) | <1 1 0> | <1 1 0> | 142.2 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 71.1 |
Te2W (mp-22693) | <1 1 0> | <1 1 0> | 213.4 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 50.3 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
73 | 67 | 67 | 0 | 0 | 0 |
67 | 73 | 67 | 0 | 0 | 0 |
67 | 67 | 73 | 0 | 0 | 0 |
0 | 0 | 0 | 31 | 0 | 0 |
0 | 0 | 0 | 0 | 31 | 0 |
0 | 0 | 0 | 0 | 0 | 31 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
106.1 | -50.6 | -50.6 | 0 | 0 | 0 |
-50.6 | 106.1 | -50.6 | 0 | 0 | 0 |
-50.6 | -50.6 | 106.1 | 0 | 0 | 0 |
0 | 0 | 0 | 31.8 | 0 | 0 |
0 | 0 | 0 | 0 | 31.8 | 0 |
0 | 0 | 0 | 0 | 0 | 31.8 |
Shear Modulus GV20 GPa |
Bulk Modulus KV69 GPa |
Shear Modulus GR7 GPa |
Bulk Modulus KR69 GPa |
Shear Modulus GVRH14 GPa |
Bulk Modulus KVRH69 GPa |
Elastic Anisotropy9.56 |
Poisson's Ratio0.41 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Tm2AgHg (mp-979176) | 0.0000 | 0.002 | 3 |
Gd2AgRh (mp-1006068) | 0.0000 | 0.027 | 3 |
Li2CaPb (mp-865892) | 0.0000 | 0.000 | 3 |
TaMnRu2 (mp-867811) | 0.0000 | 0.000 | 3 |
La2ZnRu (mp-867847) | 0.0000 | 0.058 | 3 |
LiMgSnPd (mp-7555) | 0.0000 | 0.000 | 4 |
LiMgSnAu (mp-7554) | 0.0000 | 0.058 | 4 |
LiMgSbPt (mp-571584) | 0.0000 | 0.086 | 4 |
LiMgSbPd (mp-10179) | 0.0000 | 0.074 | 4 |
LiMgSnPt (mp-11806) | 0.0000 | 0.000 | 4 |
Ga3Au (mp-983412) | 0.0000 | 0.146 | 2 |
GaSi3 (mp-983359) | 0.0000 | 0.466 | 2 |
SmTa3 (mp-972514) | 0.0000 | 0.481 | 2 |
Re3Sb (mp-974417) | 0.0000 | 0.633 | 2 |
Mn3Ge (mp-865027) | 0.0000 | 0.000 | 2 |
Br (mp-673171) | 0.0000 | 0.630 | 1 |
Ti (mp-73) | 0.0000 | 0.112 | 1 |
I (mp-684663) | 0.0000 | 0.446 | 1 |
Cr (mp-90) | 0.0000 | 0.000 | 1 |
Bi (mp-568610) | 0.0000 | 0.139 | 1 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ho_3 Ag Hg |
Final Energy/Atom-2.3349 eV |
Corrected Energy-9.3397 eV
-9.3397 eV = -9.3397 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)