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-3.559 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.002 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. |
Density5.29 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToYNbO4 |
Band Gap3.667 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 MauguinI41/a [88] |
HallI 4bw 1bw |
Point Group4/m |
Crystal Systemtetragonal |
Topological Classificationtrivial*
|
SubclassificationLCEBR†
|
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%)
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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Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
4.92 | -0.00 | -0.00 |
0.00 | 4.92 | 0.00 |
0.00 | 0.00 | 4.59 |
Dielectric Tensor εij (total) |
||
---|---|---|
21.81 | -0.00 | -0.00 |
0.00 | 21.81 | 0.00 |
0.00 | 0.00 | 14.58 |
Polycrystalline dielectric constant
εpoly∞
4.81
|
Polycrystalline dielectric constant
εpoly
19.40
|
Refractive Index n2.19 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
CaZnF4 (mp-5104) | 0.2155 | 0.004 | 3 |
SrZnF4 (mp-5078) | 0.1748 | 0.000 | 3 |
DyWO4 (mp-769941) | 0.2263 | 0.145 | 3 |
CeNbO4 (mp-557564) | 0.1714 | 0.002 | 3 |
DyNbO4 (mp-1095234) | 0.1156 | 0.002 | 3 |
KEu(MoO4)2 (mp-647282) | 0.6695 | 0.316 | 4 |
CsPr(MoO4)2 (mp-649915) | 0.7282 | 0.000 | 4 |
Cr2AgBiO8 (mp-565669) | 0.6567 | 0.011 | 4 |
Li2CaHfF8 (mp-16577) | 0.6691 | 0.000 | 4 |
KEu(MoO4)2 (mp-566325) | 0.6568 | 0.000 | 4 |
TlCl2 (mp-27205) | 0.3212 | 0.000 | 2 |
TlBr2 (mp-27398) | 0.4681 | 0.000 | 2 |
InI2 (mp-29312) | 0.5045 | 0.000 | 2 |
InBr2 (mp-568108) | 0.4963 | 0.000 | 2 |
GaCl2 (mp-568848) | 0.5657 | 0.000 | 2 |
Ca2YAs(WO6)2 (mp-562728) | 0.7384 | 0.000 | 5 |
Run TypeGGA |
Energy Cutoff700 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Y_sv Nb_pv O |
Final Energy/Atom-9.1507 eV |
Corrected Energy-115.3045 eV
Uncorrected energy = -109.8085 eV
Composition-based energy adjustment (-0.687 eV/atom x 8.0 atoms) = -5.4960 eV
Corrected energy = -115.3045 eV
|
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)