Final Magnetic Moment0.189 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-0.019 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. |
Density18.53 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 MauguinCmcm [63] |
Hall-C 2c 2 |
Point Groupmmm |
Crystal Systemorthorhombic |
Topological ClassificationTI*
|
SubclassificationNLC†
|
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] |
---|---|---|---|
AlN (mp-661) | <1 0 1> | <0 1 0> | 243.0 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 267.4 |
AlN (mp-661) | <1 1 1> | <0 1 0> | 194.4 |
GaAs (mp-2534) | <1 0 0> | <0 1 0> | 243.0 |
GaAs (mp-2534) | <1 1 0> | <0 1 0> | 48.6 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 158.3 |
BaF2 (mp-1029) | <1 1 0> | <0 1 1> | 215.2 |
BaF2 (mp-1029) | <1 1 1> | <1 0 1> | 274.4 |
GaN (mp-804) | <0 0 1> | <0 1 0> | 243.0 |
GaN (mp-804) | <1 0 0> | <0 1 0> | 340.2 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 211.0 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 316.5 |
GaN (mp-804) | <1 1 1> | <0 0 1> | 263.8 |
SiO2 (mp-6930) | <1 0 0> | <1 0 1> | 274.4 |
SiO2 (mp-6930) | <1 0 1> | <0 1 0> | 145.8 |
SiO2 (mp-6930) | <1 1 1> | <0 1 1> | 215.2 |
KCl (mp-23193) | <1 0 0> | <0 0 1> | 158.3 |
KCl (mp-23193) | <1 1 0> | <1 0 0> | 224.2 |
KCl (mp-23193) | <1 1 1> | <1 0 1> | 274.4 |
DyScO3 (mp-31120) | <0 0 1> | <0 1 0> | 97.2 |
DyScO3 (mp-31120) | <1 0 0> | <0 1 1> | 143.4 |
DyScO3 (mp-31120) | <1 0 1> | <0 1 1> | 286.9 |
DyScO3 (mp-31120) | <1 1 0> | <0 0 1> | 316.5 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 158.3 |
InAs (mp-20305) | <1 1 0> | <0 1 1> | 215.2 |
InAs (mp-20305) | <1 1 1> | <1 0 1> | 274.4 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 263.8 |
ZnSe (mp-1190) | <1 1 0> | <0 1 0> | 48.6 |
ZnSe (mp-1190) | <1 1 1> | <0 1 0> | 340.2 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 158.3 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 211.0 |
KTaO3 (mp-3614) | <1 1 1> | <0 1 0> | 340.2 |
CdS (mp-672) | <0 0 1> | <0 1 0> | 243.0 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 224.2 |
CdS (mp-672) | <1 0 1> | <1 0 0> | 298.9 |
LiF (mp-1138) | <1 0 0> | <0 0 1> | 263.8 |
LiF (mp-1138) | <1 1 0> | <0 1 0> | 48.6 |
Te2W (mp-22693) | <0 1 1> | <1 1 0> | 178.3 |
YVO4 (mp-19133) | <1 0 1> | <1 1 1> | 207.1 |
Ag (mp-124) | <1 0 0> | <0 1 0> | 243.0 |
Ag (mp-124) | <1 1 0> | <0 1 0> | 48.6 |
Ag (mp-124) | <1 1 1> | <0 1 0> | 243.0 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 1> | 274.4 |
GaSe (mp-1943) | <0 0 1> | <0 1 1> | 215.2 |
GaSe (mp-1943) | <1 0 0> | <0 0 1> | 211.0 |
GaSe (mp-1943) | <1 0 1> | <0 0 1> | 211.0 |
BN (mp-984) | <0 0 1> | <1 0 0> | 224.2 |
BN (mp-984) | <1 0 0> | <0 0 1> | 211.0 |
BN (mp-984) | <1 0 1> | <0 1 0> | 243.0 |
BN (mp-984) | <1 1 0> | <0 1 0> | 340.2 |
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 |
---|---|---|---|
U2AlCu3 (mp-7775) | 0.6643 | 0.155 | 3 |
U2Cr3Si (mp-9394) | 0.5566 | 0.136 | 3 |
U2AlCo3 (mp-30176) | 0.6225 | 0.055 | 3 |
Gd3(AlNi3)2 (mp-580327) | 0.6903 | 0.000 | 3 |
U2Fe3Ge (mp-20917) | 0.5931 | 0.000 | 3 |
UAl2 (mp-569744) | 0.6175 | 0.000 | 2 |
Zr2Ni7 (mp-2717) | 0.7260 | 0.000 | 2 |
URe2 (mp-19890) | 0.5298 | 0.016 | 2 |
SiAg2 (mp-1095654) | 0.6566 | 0.513 | 2 |
LaMg2 (mp-1095697) | 0.5985 | 0.026 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: U Re_pv |
Final Energy/Atom-12.0791 eV |
Corrected Energy-144.9494 eV
-144.9494 eV = -144.9494 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)