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-0.138 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. |
Density6.73 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap1.092 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 MauguinP21/c [14] |
Hall-P 2ybc |
Point Group2/m |
Crystal Systemmonoclinic |
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%)
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.
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substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <0 0 1> | <1 0 0> | 306.8 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 0> | 306.8 |
AlN (mp-661) | <0 0 1> | <0 1 0> | 227.2 |
AlN (mp-661) | <1 0 0> | <0 0 1> | 233.7 |
AlN (mp-661) | <1 0 1> | <0 1 0> | 227.2 |
AlN (mp-661) | <1 1 0> | <0 1 0> | 340.8 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 61.4 |
CeO2 (mp-20194) | <1 1 0> | <0 0 1> | 175.2 |
CeO2 (mp-20194) | <1 1 1> | <1 0 0> | 306.8 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 306.8 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 61.4 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 306.8 |
CdS (mp-672) | <0 0 1> | <0 1 1> | 244.4 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 306.8 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 306.8 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 306.8 |
GaN (mp-804) | <1 1 1> | <0 1 1> | 244.4 |
DyScO3 (mp-31120) | <0 1 0> | <0 0 1> | 175.2 |
DyScO3 (mp-31120) | <1 0 0> | <0 0 1> | 175.2 |
DyScO3 (mp-31120) | <1 0 1> | <0 1 1> | 163.0 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 306.8 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 184.1 |
CdS (mp-672) | <1 0 1> | <1 0 -1> | 220.4 |
CdS (mp-672) | <1 1 0> | <0 1 0> | 340.8 |
CdS (mp-672) | <1 1 1> | <0 1 1> | 163.0 |
Te2W (mp-22693) | <0 1 1> | <0 1 1> | 244.4 |
Te2W (mp-22693) | <1 0 0> | <1 0 -1> | 293.8 |
TePb (mp-19717) | <1 1 0> | <0 1 1> | 244.4 |
Te2Mo (mp-602) | <0 0 1> | <1 1 -1> | 185.7 |
Te2Mo (mp-602) | <1 1 0> | <1 0 -1> | 293.8 |
Te2Mo (mp-602) | <1 1 1> | <0 1 0> | 284.0 |
Ag (mp-124) | <1 0 0> | <1 1 -1> | 278.6 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 175.2 |
GaSe (mp-1943) | <0 0 1> | <1 0 0> | 306.8 |
GaSe (mp-1943) | <1 0 0> | <1 0 1> | 284.0 |
GaSe (mp-1943) | <1 0 1> | <1 0 1> | 284.0 |
BN (mp-984) | <0 0 1> | <0 1 0> | 284.0 |
BN (mp-984) | <1 0 0> | <0 0 1> | 58.4 |
BN (mp-984) | <1 0 1> | <0 1 0> | 340.8 |
BN (mp-984) | <1 1 0> | <0 0 1> | 175.2 |
BN (mp-984) | <1 1 1> | <0 0 1> | 233.7 |
LiNbO3 (mp-3731) | <1 0 1> | <0 0 1> | 233.7 |
Bi2Se3 (mp-541837) | <0 0 1> | <0 1 1> | 244.4 |
MoS2 (mp-1434) | <0 0 1> | <0 1 0> | 284.0 |
Al (mp-134) | <1 1 0> | <1 0 0> | 184.1 |
LiGaO2 (mp-5854) | <1 0 1> | <1 0 0> | 184.1 |
LiGaO2 (mp-5854) | <1 1 0> | <0 0 1> | 292.1 |
TeO2 (mp-2125) | <0 0 1> | <1 0 -1> | 220.4 |
TeO2 (mp-2125) | <0 1 1> | <1 0 0> | 306.8 |
TeO2 (mp-2125) | <1 0 0> | <1 0 1> | 284.0 |
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) |
||
---|---|---|
5.49 | 0.00 | -1.46 |
0.00 | 13.22 | 0.00 |
-1.46 | 0.00 | 12.40 |
Dielectric Tensor εij (total) |
||
---|---|---|
6.20 | 0.00 | -1.28 |
0.00 | 22.10 | 0.00 |
-1.28 | 0.00 | 17.48 |
Polycrystalline dielectric constant
εpoly∞
10.37
|
Polycrystalline dielectric constant
εpoly
15.26
|
Refractive Index n3.22 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Yb2S2O (mp-22399) | 0.7077 | 0.236 | 3 |
InTeCl (mp-504630) | 0.6481 | 0.000 | 3 |
Pd(PbCl3)2 (mp-28982) | 0.7182 | 0.005 | 3 |
Tl2TeO3 (mp-543028) | 0.6469 | 0.000 | 3 |
Hg2MoO4 (mp-566907) | 0.6845 | 0.007 | 3 |
SrHBrO (mp-1080045) | 0.7466 | 0.000 | 4 |
BiTeIO3 (mp-559332) | 0.7419 | 0.007 | 4 |
AgSbPbS3 (mp-560848) | 0.6936 | 0.016 | 4 |
AgAsPbS3 (mp-22665) | 0.5670 | 0.000 | 4 |
PtCl2 (mp-684670) | 0.7383 | 0.293 | 2 |
TeI (mp-23273) | 0.6832 | 0.017 | 2 |
Run TypeGGA |
Energy Cutoff700 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Te Au I |
Final Energy/Atom-2.7856 eV |
Corrected Energy-33.4268 eV
-33.4268 eV = -33.4268 eV (uncorrected energy)
|
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)