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-1.181 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. |
Density4.63 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.833 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 MauguinC2 [5] |
HallC 2y |
Point Group2 |
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] |
---|---|---|---|
DyScO3 (mp-31120) | <0 0 1> | <1 0 -1> | 340.4 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 -1> | 226.9 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 317.7 |
ZnSe (mp-1190) | <1 1 0> | <1 1 -1> | 184.0 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 -1> | 113.5 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 317.7 |
CdS (mp-672) | <1 0 1> | <1 0 -1> | 226.9 |
CdS (mp-672) | <1 1 0> | <1 0 -1> | 283.7 |
LiF (mp-1138) | <1 0 0> | <1 0 1> | 101.1 |
LiF (mp-1138) | <1 1 0> | <1 0 0> | 158.9 |
LaAlO3 (mp-2920) | <0 0 1> | <1 0 -1> | 226.9 |
LaAlO3 (mp-2920) | <1 0 0> | <1 0 0> | 211.8 |
Te2Mo (mp-602) | <0 0 1> | <1 0 -1> | 226.9 |
Ag (mp-124) | <1 1 0> | <1 0 -1> | 283.7 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 0 -1> | 226.9 |
LaAlO3 (mp-2920) | <1 0 1> | <1 0 -1> | 226.9 |
AlN (mp-661) | <0 0 1> | <1 0 -1> | 226.9 |
AlN (mp-661) | <1 0 0> | <1 0 1> | 202.1 |
AlN (mp-661) | <1 1 1> | <0 0 1> | 250.1 |
GaAs (mp-2534) | <1 0 0> | <1 0 -1> | 226.9 |
GaAs (mp-2534) | <1 1 0> | <1 1 -1> | 184.0 |
Al (mp-134) | <1 0 0> | <1 0 -1> | 113.5 |
Al (mp-134) | <1 1 0> | <1 0 -1> | 113.5 |
LiGaO2 (mp-5854) | <0 1 0> | <1 0 0> | 264.8 |
GaN (mp-804) | <0 0 1> | <1 0 -1> | 226.9 |
GaN (mp-804) | <1 0 0> | <0 0 1> | 250.1 |
GaN (mp-804) | <1 0 1> | <0 0 1> | 187.6 |
CdTe (mp-406) | <1 0 0> | <1 0 0> | 264.8 |
CdTe (mp-406) | <1 1 1> | <1 0 -1> | 226.9 |
TeO2 (mp-2125) | <1 1 1> | <1 0 0> | 105.9 |
SiO2 (mp-6930) | <0 0 1> | <1 0 0> | 264.8 |
SiO2 (mp-6930) | <1 0 1> | <1 0 -1> | 283.7 |
ZnSe (mp-1190) | <1 0 0> | <1 0 -1> | 226.9 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 -1> | 113.5 |
MgO (mp-1265) | <1 1 0> | <1 0 -1> | 283.7 |
MgO (mp-1265) | <1 1 1> | <1 0 -1> | 226.9 |
TiO2 (mp-2657) | <1 0 0> | <1 0 0> | 211.8 |
Te2W (mp-22693) | <0 0 1> | <1 0 -1> | 283.7 |
C (mp-66) | <1 0 0> | <1 0 0> | 317.7 |
C (mp-66) | <1 1 0> | <1 0 -1> | 283.7 |
C (mp-66) | <1 1 1> | <1 0 0> | 264.8 |
GdScO3 (mp-5690) | <0 1 0> | <1 0 -1> | 226.9 |
GdScO3 (mp-5690) | <1 0 0> | <1 0 -1> | 226.9 |
GdScO3 (mp-5690) | <1 1 0> | <1 0 0> | 317.7 |
TePb (mp-19717) | <1 0 0> | <1 0 0> | 264.8 |
TePb (mp-19717) | <1 1 1> | <1 0 -1> | 226.9 |
Te2Mo (mp-602) | <1 1 0> | <0 0 1> | 187.6 |
Mg (mp-153) | <1 0 0> | <1 1 -1> | 184.0 |
Mg (mp-153) | <1 0 1> | <0 0 1> | 187.6 |
Mg (mp-153) | <1 1 0> | <1 0 0> | 317.7 |
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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Piezoelectric Tensor eij (C/m2) |
|||||
---|---|---|---|---|---|
0.00000 | 0.00000 | 0.00000 | -0.00469 | 0.00000 | -0.01643 |
0.03842 | -2.13590 | 0.04041 | 0.00000 | 0.00738 | 0.00000 |
0.00000 | 0.00000 | 0.00000 | -0.02058 | 0.00000 | -0.00516 |
Piezoelectric Modulus ‖eij‖max2.13664 C/m2 |
Crystallographic Direction vmax |
---|
-0.00000 |
-1.00000 |
-2.00000 |
Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
5.66 | -0.00 | 0.28 |
-0.00 | 5.99 | -0.00 |
0.28 | -0.00 | 5.85 |
Dielectric Tensor εij (total) |
||
---|---|---|
7.02 | -0.00 | 0.75 |
-0.00 | 9.82 | -0.00 |
0.75 | -0.00 | 7.20 |
Polycrystalline dielectric constant
εpoly∞
5.84
|
Polycrystalline dielectric constant
εpoly
8.01
|
Refractive Index n2.42 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
NbBr3O (mp-606393) | 0.2467 | 0.000 | 3 |
NbCl3O (mp-27815) | 0.5021 | 0.008 | 3 |
VNCl4 (mp-27868) | 0.5687 | 0.210 | 3 |
W2NCl8 (mp-570568) | 0.5389 | 0.000 | 3 |
NbCl3O (mp-556422) | 0.4127 | 0.000 | 3 |
HgC2(SN)2 (mp-610992) | 0.7203 | 0.235 | 4 |
NaHCN2 (mp-634434) | 0.7100 | 0.035 | 4 |
Ta2Bi4Br7O2 (mp-554564) | 0.7181 | 0.002 | 4 |
WSNCl5 (mp-558716) | 0.6119 | 0.041 | 4 |
HgC2(SeN)2 (mp-570211) | 0.6772 | 0.335 | 4 |
K3HRhC5N5O (mp-697108) | 0.7122 | 0.099 | 6 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Nb_pv I O |
Final Energy/Atom-4.9648 eV |
Corrected Energy-53.2961 eV
Uncorrected energy = -49.6481 eV
Composition-based energy adjustment (-0.687 eV/atom x 2.0 atoms) = -1.3740 eV
Composition-based energy adjustment (-0.379 eV/atom x 6.0 atoms) = -2.2740 eV
Corrected energy = -53.2961 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)