Final Magnetic Moment0.037 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-2.706 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.649 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. |
Density8.17 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToEuTaO4 |
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 MauguinP2/c [13] |
Hall-P 2yc |
Point Group2/m |
Crystal Systemmonoclinic |
Topological Classificationtrivial*
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SubclassificationLCEBR†
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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> | <0 0 1> | 209.4 |
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 149.5 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 149.5 |
AlN (mp-661) | <1 0 0> | <1 0 -1> | 202.0 |
AlN (mp-661) | <1 1 0> | <1 0 0> | 185.3 |
AlN (mp-661) | <1 1 1> | <1 0 0> | 278.0 |
AlN (mp-661) | <0 0 1> | <0 1 0> | 141.8 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 123.5 |
GaAs (mp-2534) | <1 0 0> | <1 0 -1> | 161.6 |
GaAs (mp-2534) | <1 1 1> | <1 0 1> | 227.2 |
CeO2 (mp-20194) | <1 0 0> | <1 1 -1> | 246.8 |
CeO2 (mp-20194) | <1 1 0> | <1 0 0> | 123.5 |
GaAs (mp-2534) | <1 1 0> | <1 0 1> | 45.4 |
BaF2 (mp-1029) | <1 0 0> | <0 1 0> | 283.6 |
BaF2 (mp-1029) | <1 1 0> | <0 0 1> | 329.0 |
BaF2 (mp-1029) | <1 1 1> | <0 1 1> | 206.1 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 89.7 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 29.9 |
GaN (mp-804) | <1 1 1> | <1 0 -1> | 121.2 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 119.6 |
GaN (mp-804) | <1 0 1> | <1 1 1> | 214.3 |
SiO2 (mp-6930) | <0 0 1> | <1 0 -1> | 202.0 |
SiO2 (mp-6930) | <1 0 0> | <1 0 0> | 185.3 |
SiO2 (mp-6930) | <1 0 1> | <1 0 1> | 136.3 |
SiO2 (mp-6930) | <1 1 0> | <1 0 0> | 92.7 |
KCl (mp-23193) | <1 0 0> | <0 1 0> | 283.6 |
KCl (mp-23193) | <1 1 0> | <1 0 1> | 181.8 |
KCl (mp-23193) | <1 1 1> | <1 0 -1> | 282.7 |
KTaO3 (mp-3614) | <1 0 0> | <0 1 0> | 170.1 |
CdS (mp-672) | <1 1 1> | <1 0 -1> | 202.0 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 0> | 30.9 |
LiF (mp-1138) | <1 1 1> | <1 0 1> | 227.2 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 0> | 216.2 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 216.2 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 1> | 45.4 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 -1> | 161.6 |
DyScO3 (mp-31120) | <1 1 0> | <1 1 -1> | 246.8 |
DyScO3 (mp-31120) | <1 1 1> | <0 0 1> | 269.2 |
Te2W (mp-22693) | <0 1 0> | <0 0 1> | 269.2 |
Te2W (mp-22693) | <1 0 0> | <1 0 -1> | 282.7 |
YVO4 (mp-19133) | <0 0 1> | <1 0 -1> | 202.0 |
YVO4 (mp-19133) | <1 0 0> | <1 0 -1> | 323.1 |
YVO4 (mp-19133) | <1 1 0> | <0 1 0> | 255.2 |
InAs (mp-20305) | <1 0 0> | <1 1 0> | 335.4 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 329.0 |
Te2Mo (mp-602) | <1 1 0> | <1 0 -1> | 282.7 |
ZnSe (mp-1190) | <1 0 0> | <1 0 -1> | 161.6 |
ZnSe (mp-1190) | <1 1 0> | <1 0 1> | 45.4 |
ZnSe (mp-1190) | <1 1 1> | <1 0 1> | 227.2 |
Ag (mp-124) | <1 0 0> | <1 1 0> | 209.6 |
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 |
---|---|---|---|
DyWO4 (mp-770600) | 0.2430 | 0.000 | 3 |
YTaO4 (mp-5377) | 0.2937 | 0.000 | 3 |
ZrSiO4 (mp-1020588) | 0.3034 | 0.182 | 3 |
SmTaO4 (mp-12931) | 0.3085 | 0.000 | 3 |
GdTaO4 (mp-4875) | 0.2810 | 0.000 | 3 |
YSb(WO4)2 (mvc-675) | 0.4543 | 0.157 | 4 |
YBi(WO4)2 (mvc-679) | 0.2797 | 0.003 | 4 |
YSn(WO4)2 (mvc-705) | 0.4139 | 0.065 | 4 |
YAg(WO4)2 (mvc-653) | 0.6046 | 0.008 | 4 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Eu Ta_pv O |
Final Energy/Atom-9.2282 eV |
Corrected Energy-116.3567 eV
-116.3567 eV = -110.7384 eV (uncorrected energy) - 5.6183 eV (MP Anion Correction)
|
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)