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-3.053 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. |
Density4.86 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap3.772 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 MauguinP43212 [96] |
HallP 4nw 2abw |
Point Group422 |
Crystal Systemtetragonal |
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.
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Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
CeO2 (mp-20194) | <1 0 0> | <0 0 1> | 237.2 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 284.6 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 189.8 |
SiO2 (mp-6930) | <1 0 1> | <1 0 0> | 172.8 |
DyScO3 (mp-31120) | <1 0 1> | <0 0 1> | 284.6 |
InAs (mp-20305) | <1 0 0> | <0 0 1> | 189.8 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 284.6 |
KTaO3 (mp-3614) | <1 1 0> | <0 0 1> | 332.1 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 142.3 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 86.4 |
CdS (mp-672) | <1 1 0> | <1 0 1> | 98.6 |
YVO4 (mp-19133) | <1 1 0> | <1 0 0> | 259.2 |
BN (mp-984) | <0 0 1> | <0 0 1> | 332.1 |
BN (mp-984) | <1 0 0> | <0 0 1> | 237.2 |
LiNbO3 (mp-3731) | <1 0 0> | <1 0 1> | 295.7 |
TiO2 (mp-2657) | <0 0 1> | <0 0 1> | 189.8 |
TiO2 (mp-2657) | <1 0 0> | <1 0 0> | 259.2 |
Ge3(BiO3)4 (mp-23560) | <1 0 0> | <0 0 1> | 237.2 |
GdScO3 (mp-5690) | <1 0 1> | <0 0 1> | 284.6 |
Mg (mp-153) | <1 0 1> | <1 0 0> | 172.8 |
Mg (mp-153) | <1 1 1> | <0 0 1> | 237.2 |
PbS (mp-21276) | <1 0 0> | <0 0 1> | 189.8 |
GaP (mp-2490) | <1 0 0> | <0 0 1> | 237.2 |
TbScO3 (mp-31119) | <0 1 1> | <1 1 1> | 262.1 |
Ni (mp-23) | <1 0 0> | <1 0 1> | 98.6 |
Ni (mp-23) | <1 1 1> | <0 0 1> | 332.1 |
NdGaO3 (mp-3196) | <0 1 1> | <1 1 1> | 262.1 |
NdGaO3 (mp-3196) | <1 0 1> | <1 1 1> | 262.1 |
NdGaO3 (mp-3196) | <1 1 0> | <0 0 1> | 237.2 |
SiC (mp-11714) | <0 0 1> | <0 0 1> | 332.1 |
SiC (mp-11714) | <1 0 1> | <1 0 0> | 259.2 |
Si (mp-149) | <1 0 0> | <0 0 1> | 237.2 |
CdSe (mp-2691) | <1 0 0> | <0 0 1> | 189.8 |
WS2 (mp-224) | <0 0 1> | <0 0 1> | 237.2 |
ZrO2 (mp-2858) | <1 0 -1> | <0 0 1> | 142.3 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 172.8 |
DyScO3 (mp-31120) | <0 1 1> | <1 1 1> | 262.1 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 142.3 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 1> | 295.7 |
MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 237.2 |
Al (mp-134) | <1 1 0> | <0 0 1> | 332.1 |
Al (mp-134) | <1 1 1> | <0 0 1> | 142.3 |
LiGaO2 (mp-5854) | <0 1 0> | <1 0 0> | 259.2 |
SiC (mp-7631) | <0 0 1> | <0 0 1> | 332.1 |
LiTaO3 (mp-3666) | <1 0 0> | <1 0 1> | 295.7 |
MgO (mp-1265) | <1 0 0> | <0 0 1> | 237.2 |
Mg (mp-153) | <0 0 1> | <0 0 1> | 237.2 |
KP(HO2)2 (mp-23959) | <1 0 0> | <0 0 1> | 237.2 |
TbScO3 (mp-31119) | <1 0 1> | <0 0 1> | 284.6 |
Ni (mp-23) | <1 1 0> | <0 0 1> | 237.2 |
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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Piezoelectric Tensor eij (C/m2) |
|||||
---|---|---|---|---|---|
0.00000 | 0.00000 | 0.00000 | 0.09894 | 0.00000 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | 0.00000 | -0.09894 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | 0.00000 | 0.00000 | 0.00000 |
Piezoelectric Modulus ‖eij‖max0.09894 C/m2 |
Crystallographic Direction vmax |
---|
0.00000 |
1.00000 |
0.00000 |
Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
3.76 | 0.00 | 0.00 |
0.00 | 3.76 | 0.00 |
0.00 | 0.00 | 3.71 |
Dielectric Tensor εij (total) |
||
---|---|---|
11.15 | 0.00 | 0.00 |
0.00 | 11.15 | 0.00 |
0.00 | 0.00 | 12.94 |
Polycrystalline dielectric constant
εpoly∞
3.74
|
Polycrystalline dielectric constant
εpoly
11.75
|
Refractive Index n1.94 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Dy2Ge2O7 (mp-772793) | 0.0234 | 0.016 | 3 |
Ho2Ge2O7 (mp-560082) | 0.0279 | 0.000 | 3 |
Er2Ge2O7 (mp-13643) | 0.0486 | 0.000 | 3 |
Tb2Ge2O7 (mp-14649) | 0.0113 | 0.000 | 3 |
Tm2Ge2O7 (mp-14708) | 0.0696 | 0.000 | 3 |
Er4Si3O11F2 (mp-554009) | 0.6157 | 0.007 | 4 |
Er3Si3O10F (mp-542038) | 0.5365 | 0.006 | 4 |
Dy3Si3O10F (mp-16164) | 0.5569 | 0.000 | 4 |
Ho3Si3O10F (mp-16165) | 0.5491 | 0.000 | 4 |
Y3Si3O10F (mp-14630) | 0.5635 | 0.012 | 4 |
KHoCoSi2O7 (mp-735519) | 0.6839 | 0.064 | 5 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Y_sv Ge_d O |
Final Energy/Atom-7.7703 eV |
Corrected Energy-361.1273 eV
Uncorrected energy = -341.8913 eV
Composition-based energy adjustment (-0.687 eV/atom x 28.0 atoms) = -19.2360 eV
Corrected energy = -361.1273 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)