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-3.269 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.009 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. |
Density1.81 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToSiO2 |
Band Gap5.627 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 MauguinP6522 [179] |
HallP 65 2 (0 0 1) |
Point Group622 |
Crystal Systemhexagonal |
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] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <0 0 1> | 328.6 |
AlN (mp-661) | <0 0 1> | <1 1 0> | 269.8 |
AlN (mp-661) | <1 0 1> | <0 0 1> | 234.7 |
AlN (mp-661) | <1 1 0> | <0 0 1> | 328.6 |
BaF2 (mp-1029) | <1 0 0> | <0 0 1> | 234.7 |
GaN (mp-804) | <0 0 1> | <0 0 1> | 187.8 |
GaN (mp-804) | <1 0 0> | <1 1 0> | 269.8 |
SiO2 (mp-6930) | <1 0 0> | <0 0 1> | 328.6 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 179.8 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 207.7 |
KCl (mp-23193) | <1 1 0> | <0 0 1> | 234.7 |
InAs (mp-20305) | <1 1 1> | <0 0 1> | 187.8 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 1> | 280.0 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 207.7 |
KTaO3 (mp-3614) | <1 1 1> | <0 0 1> | 187.8 |
CdS (mp-672) | <0 0 1> | <0 0 1> | 46.9 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 207.7 |
CdS (mp-672) | <1 1 0> | <1 0 0> | 51.9 |
LiF (mp-1138) | <1 0 0> | <1 0 1> | 280.0 |
LiF (mp-1138) | <1 1 0> | <1 0 0> | 207.7 |
LiF (mp-1138) | <1 1 1> | <0 0 1> | 328.6 |
Te2W (mp-22693) | <0 0 1> | <1 1 0> | 89.9 |
Te2W (mp-22693) | <1 1 1> | <0 0 1> | 234.7 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 51.9 |
YVO4 (mp-19133) | <1 0 0> | <1 1 0> | 89.9 |
YVO4 (mp-19133) | <1 0 1> | <1 0 0> | 207.7 |
TePb (mp-19717) | <1 0 0> | <0 0 1> | 328.6 |
TePb (mp-19717) | <1 1 0> | <0 0 1> | 234.7 |
Te2Mo (mp-602) | <0 0 1> | <0 0 1> | 140.8 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 328.6 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 46.9 |
GdScO3 (mp-5690) | <0 0 1> | <1 0 0> | 259.6 |
GdScO3 (mp-5690) | <1 0 1> | <1 0 1> | 280.0 |
Mg (mp-153) | <0 0 1> | <0 0 1> | 140.8 |
Mg (mp-153) | <1 0 0> | <1 1 0> | 269.8 |
KP(HO2)2 (mp-23959) | <0 1 0> | <1 0 0> | 155.7 |
KP(HO2)2 (mp-23959) | <0 1 1> | <1 0 0> | 103.8 |
LaF3 (mp-905) | <1 0 0> | <1 0 0> | 51.9 |
PbS (mp-21276) | <1 1 1> | <0 0 1> | 187.8 |
Ni (mp-23) | <1 1 1> | <0 0 1> | 187.8 |
InSb (mp-20012) | <1 1 0> | <1 0 0> | 311.5 |
PbSe (mp-2201) | <1 1 0> | <0 0 1> | 328.6 |
BaTiO3 (mp-5986) | <1 0 1> | <1 0 0> | 259.6 |
BaTiO3 (mp-5986) | <1 1 0> | <1 0 0> | 259.6 |
BaTiO3 (mp-5986) | <1 1 1> | <1 1 1> | 202.9 |
NdGaO3 (mp-3196) | <1 0 1> | <0 0 1> | 328.6 |
CdSe (mp-2691) | <1 1 0> | <0 0 1> | 328.6 |
WS2 (mp-224) | <0 0 1> | <0 0 1> | 140.8 |
WS2 (mp-224) | <1 0 0> | <1 0 0> | 311.5 |
C (mp-48) | <1 1 1> | <1 1 1> | 101.4 |
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 | 0.00233 | 0.00000 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | 0.00000 | -0.00233 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | 0.00000 | 0.00000 | 0.00000 |
Piezoelectric Modulus ‖eij‖max0.00233 C/m2 |
Crystallographic Direction vmax |
---|
-1.00000 |
-1.00000 |
0.00000 |
Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
2.00 | -0.00 | 0.00 |
-0.00 | 2.00 | 0.00 |
0.00 | 0.00 | 2.01 |
Dielectric Tensor εij (total) |
||
---|---|---|
3.53 | -0.00 | 0.00 |
-0.00 | 3.53 | 0.00 |
0.00 | 0.00 | 3.65 |
Polycrystalline dielectric constant
εpoly∞
2.00
|
Polycrystalline dielectric constant
εpoly
3.57
|
Refractive Index n1.41 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
AlPO4 (mp-5724) | 0.5063 | 0.003 | 3 |
AlPO4 (mp-5859) | 0.4684 | 0.011 | 3 |
AlPO4 (mp-37990) | 0.4274 | 0.014 | 3 |
AlPO4 (mp-557842) | 0.4269 | 0.011 | 3 |
AlPO4 (mp-675254) | 0.4029 | 0.012 | 3 |
CsAlSiO4 (mp-561457) | 0.6393 | 0.000 | 4 |
CsBePO4 (mp-15395) | 0.5720 | 0.000 | 4 |
CrN2 (mp-1016070) | 0.1295 | 0.339 | 2 |
SiO2 (mp-555891) | 0.2098 | 0.008 | 2 |
CrN2 (mp-1096919) | 0.1652 | 0.348 | 2 |
CrN2 (mp-1096951) | 0.2364 | 0.342 | 2 |
CrN2 (mp-1096913) | 0.1441 | 0.342 | 2 |
C (mp-1095534) | 0.7438 | 1.121 | 1 |
Explore more synthesis descriptions for materials of composition SiO2.
Text computed by synthesisproject.org.
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Si O |
Final Energy/Atom-7.9068 eV |
Corrected Energy-150.7504 eV
-150.7504 eV = -142.3229 eV (uncorrected energy) - 8.4275 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)