Final Magnetic Moment1.000 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-2.980 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. |
Density8.91 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap1.985 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 |
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] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <1 0 0> | 148.1 |
LaAlO3 (mp-2920) | <1 0 0> | <0 0 1> | 144.6 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 148.1 |
LaAlO3 (mp-2920) | <1 1 0> | <0 0 1> | 260.3 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 86.8 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 173.5 |
AlN (mp-661) | <1 0 1> | <1 0 0> | 118.5 |
AlN (mp-661) | <1 1 1> | <1 0 -1> | 116.3 |
AlN (mp-661) | <1 1 0> | <1 0 -1> | 193.9 |
CeO2 (mp-20194) | <1 1 0> | <1 0 1> | 43.9 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 29.6 |
GaN (mp-804) | <0 0 1> | <1 0 0> | 88.9 |
GaN (mp-804) | <1 0 1> | <1 1 1> | 155.4 |
GaN (mp-804) | <1 1 0> | <0 0 1> | 28.9 |
SiO2 (mp-6930) | <1 0 0> | <1 0 -1> | 193.9 |
SiO2 (mp-6930) | <1 0 1> | <1 1 1> | 259.0 |
KCl (mp-23193) | <1 0 0> | <1 1 1> | 259.0 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 266.6 |
BaF2 (mp-1029) | <1 0 0> | <0 1 0> | 275.2 |
BaF2 (mp-1029) | <1 1 0> | <1 0 1> | 175.5 |
DyScO3 (mp-31120) | <1 0 0> | <1 1 1> | 310.7 |
DyScO3 (mp-31120) | <1 1 1> | <0 1 1> | 279.5 |
InAs (mp-20305) | <1 0 0> | <1 1 -1> | 190.2 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 115.7 |
GaN (mp-804) | <1 1 1> | <1 0 -1> | 155.1 |
ZnSe (mp-1190) | <1 1 0> | <1 1 1> | 310.7 |
SiO2 (mp-6930) | <0 0 1> | <1 0 -1> | 193.9 |
SiO2 (mp-6930) | <1 1 0> | <0 0 1> | 144.6 |
SiO2 (mp-6930) | <1 1 1> | <0 0 1> | 260.3 |
KCl (mp-23193) | <1 1 0> | <1 0 1> | 175.5 |
KTaO3 (mp-3614) | <1 0 0> | <0 1 0> | 192.6 |
DyScO3 (mp-31120) | <0 0 1> | <1 0 1> | 131.6 |
DyScO3 (mp-31120) | <0 1 0> | <1 0 1> | 43.9 |
DyScO3 (mp-31120) | <0 1 1> | <1 0 0> | 207.4 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 1> | 307.1 |
CdS (mp-672) | <0 0 1> | <1 0 0> | 237.0 |
CdS (mp-672) | <1 0 1> | <1 0 1> | 219.4 |
CdS (mp-672) | <1 1 0> | <1 0 -1> | 155.1 |
CdS (mp-672) | <1 1 1> | <1 0 1> | 263.2 |
InAs (mp-20305) | <1 1 0> | <0 0 1> | 318.2 |
InAs (mp-20305) | <1 1 1> | <0 1 1> | 199.6 |
LiF (mp-1138) | <1 1 0> | <1 0 1> | 263.2 |
ZnSe (mp-1190) | <1 0 0> | <1 0 1> | 131.6 |
ZnSe (mp-1190) | <1 1 1> | <1 0 1> | 219.4 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 88.9 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 1> | 219.4 |
Te2W (mp-22693) | <0 0 1> | <1 1 0> | 242.6 |
CdS (mp-672) | <1 0 0> | <1 0 -1> | 116.3 |
YVO4 (mp-19133) | <0 0 1> | <0 1 0> | 302.7 |
YVO4 (mp-19133) | <1 1 0> | <0 1 0> | 247.7 |
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 |
---|---|---|---|
DyTaO4 (mp-7703) | 0.2053 | 0.000 | 3 |
HoTaO4 (mp-5985) | 0.2052 | 0.000 | 3 |
YTaO4 (mp-5377) | 0.1820 | 0.000 | 3 |
SmTaO4 (mp-12931) | 0.2032 | 0.000 | 3 |
GdTaO4 (mp-4875) | 0.1906 | 0.000 | 3 |
ErAg(WO4)2 (mp-19655) | 0.6905 | 0.002 | 4 |
YSb(WO4)2 (mvc-675) | 0.4646 | 0.157 | 4 |
YBi(WO4)2 (mvc-679) | 0.3768 | 0.003 | 4 |
YSn(WO4)2 (mvc-705) | 0.4658 | 0.065 | 4 |
ZrTe5 (mp-605) | 0.7433 | 0.000 | 2 |
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesW: 6.2 eV |
PseudopotentialsVASP PAW: Dy_3 W_pv O |
Final Energy/Atom-8.0126 eV |
Corrected Energy-110.4709 eV
-110.4709 eV = -96.1506 eV (uncorrected energy) - 8.7020 eV (MP Advanced Correction) - 5.6183 eV (MP Anion Correction)
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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)