Final Magnetic Moment3.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-2.477 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. |
Density3.53 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap1.211 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 MauguinR3m [166] |
Hall-R 3 2" |
Point Group3m |
Crystal Systemtrigonal |
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> | <1 0 0> | 309.4 |
LaAlO3 (mp-2920) | <1 0 1> | <0 0 1> | 216.8 |
AlN (mp-661) | <0 0 1> | <0 0 1> | 162.6 |
AlN (mp-661) | <1 1 0> | <1 1 1> | 240.2 |
AlN (mp-661) | <1 1 1> | <1 0 0> | 247.5 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 61.9 |
CeO2 (mp-20194) | <1 1 0> | <1 1 0> | 214.3 |
CeO2 (mp-20194) | <1 1 1> | <0 0 1> | 54.2 |
GaAs (mp-2534) | <1 0 0> | <0 0 1> | 162.6 |
GaAs (mp-2534) | <1 1 0> | <1 0 0> | 185.6 |
GaAs (mp-2534) | <1 1 1> | <0 0 1> | 54.2 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 309.4 |
BaF2 (mp-1029) | <1 1 1> | <1 1 0> | 214.3 |
GaN (mp-804) | <1 0 0> | <1 0 0> | 247.5 |
KCl (mp-23193) | <1 1 1> | <1 1 0> | 214.3 |
DyScO3 (mp-31120) | <0 1 0> | <1 1 0> | 214.3 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 185.6 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 61.9 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 309.4 |
ZnSe (mp-1190) | <1 0 0> | <0 0 1> | 162.6 |
ZnSe (mp-1190) | <1 1 0> | <1 0 0> | 185.6 |
ZnSe (mp-1190) | <1 1 1> | <0 0 1> | 54.2 |
KTaO3 (mp-3614) | <1 0 0> | <0 0 1> | 162.6 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 185.6 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 309.4 |
CdS (mp-672) | <1 1 1> | <1 0 0> | 247.5 |
TePb (mp-19717) | <1 1 1> | <1 1 0> | 214.3 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 309.4 |
Ag (mp-124) | <1 1 1> | <1 1 0> | 214.3 |
Bi2Te3 (mp-34202) | <0 0 1> | <0 0 1> | 216.8 |
GaSe (mp-1943) | <0 0 1> | <0 0 1> | 162.6 |
BN (mp-984) | <0 0 1> | <1 0 0> | 309.4 |
BN (mp-984) | <1 0 0> | <1 1 0> | 214.3 |
BN (mp-984) | <1 0 1> | <0 0 1> | 216.8 |
BN (mp-984) | <1 1 0> | <1 0 0> | 309.4 |
BN (mp-984) | <1 1 1> | <1 0 0> | 247.5 |
LiNbO3 (mp-3731) | <0 0 1> | <0 0 1> | 162.6 |
Al (mp-134) | <1 0 0> | <0 0 1> | 162.6 |
Al (mp-134) | <1 1 0> | <1 0 0> | 185.6 |
LiGaO2 (mp-5854) | <1 0 1> | <1 0 0> | 185.6 |
CdTe (mp-406) | <1 1 1> | <0 0 1> | 216.8 |
TeO2 (mp-2125) | <1 0 1> | <1 1 1> | 240.2 |
SiC (mp-7631) | <1 0 0> | <1 0 0> | 247.5 |
SiC (mp-7631) | <1 0 1> | <1 0 0> | 247.5 |
SiC (mp-7631) | <1 1 0> | <1 0 0> | 247.5 |
LiTaO3 (mp-3666) | <0 0 1> | <0 0 1> | 162.6 |
LiTaO3 (mp-3666) | <1 0 0> | <1 1 0> | 214.3 |
MgO (mp-1265) | <1 0 0> | <1 0 0> | 309.4 |
MgO (mp-1265) | <1 1 0> | <1 0 0> | 309.4 |
MgO (mp-1265) | <1 1 1> | <1 1 0> | 214.3 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
42 | 21 | 14 | 0 | 0 | 0 |
21 | 42 | 14 | -0 | 0 | 0 |
14 | 14 | 5 | 0 | 0 | 0 |
0 | -0 | 0 | 3 | 0 | 0 |
0 | 0 | 0 | 0 | 3 | 0 |
0 | 0 | 0 | 0 | 0 | 10 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
4.6 | -45 | 126 | -6.9 | 0 | 0 |
-45 | 4.6 | 126 | 6.9 | 0 | 0 |
126 | 126 | -564.3 | 0 | 0 | 0 |
-6.9 | 6.9 | 0 | 287.8 | 0 | 0 |
0 | 0 | 0 | 0 | 287.8 | -13.9 |
0 | 0 | 0 | 0 | -13.9 | 99.2 |
Shear Modulus GV6 GPa |
Bulk Modulus KV21 GPa |
Shear Modulus GR-15 GPa |
Bulk Modulus KR-7 GPa |
Shear Modulus GVRH-4 GPa |
Bulk Modulus KVRH7 GPa |
Elastic Anisotropy-10.97 |
Poisson's Ratio0.90 |
Dielectric Tensor εij∞ (electronic contribution) |
||
---|---|---|
2.32 | 0.00 | -0.00 |
0.00 | 2.32 | -0.00 |
-0.00 | -0.00 | 2.41 |
Dielectric Tensor εij (total) |
||
---|---|---|
5.88 | 0.00 | -0.00 |
0.00 | 5.88 | -0.00 |
-0.00 | -0.00 | 6.16 |
Polycrystalline dielectric constant
εpoly∞
2.35
|
Polycrystalline dielectric constant
εpoly
5.98
|
Refractive Index n1.53 |
Potentially ferroelectric?Unknown |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
TlSbF6 (mp-8348) | 0.1029 | 0.000 | 3 |
BaSiF6 (mp-5588) | 0.1435 | 0.000 | 3 |
CsRuF6 (mp-8015) | 0.1638 | 0.000 | 3 |
KRuF6 (mp-8013) | 0.1197 | 0.000 | 3 |
KAsF6 (mp-7569) | 0.1240 | 0.000 | 3 |
Cs2TlSiH6 (mp-989560) | 0.6712 | 0.015 | 4 |
Cs2SeClF6 (mp-989544) | 0.6860 | 0.000 | 4 |
BaMg2FeH8 (mp-643264) | 0.7178 | 0.000 | 4 |
SrMg2FeH8 (mp-643004) | 0.7215 | 0.000 | 4 |
LiMgH6Ir (mp-866640) | 0.6146 | 0.000 | 4 |
Rb19O3 (mp-779582) | 0.6002 | 0.043 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Rb_sv Ru_pv F |
Final Energy/Atom-4.8240 eV |
Corrected Energy-41.3637 eV
Uncorrected energy = -38.5917 eV
Composition-based energy adjustment (-0.462 eV/atom x 6.0 atoms) = -2.7720 eV
Corrected energy = -41.3637 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)