material
Sr5Li25La7Nb8O48
ID:
mp-686239
DOI:
10.17188/1284307
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 OrderingNon-magnetic |
Formation Energy / Atom-2.884 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.100 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. |
Density4.40 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToSr4Nb2O9 + La2O3 + Li8Nb2O9 + SrO |
Band Gap3.211 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 MauguinP1 [1] |
HallP 1 |
Point Group1 |
Crystal Systemtriclinic |
Band Structure
Density of States
sign indicates spin ↑ ↓
- Cu
- Ag
- Mo
- Fe
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%)
Substrates
Reference for minimal coincident interface area (MCIA) and elastic energy:substrate orientation:
| substrate material | substrate orientation | film orientation | MCIA† [Å2] |
|---|---|---|---|
| KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 250.0 |
| TePb (mp-19717) | <1 1 0> | <0 1 0> | 122.7 |
| Bi2Te3 (mp-34202) | <0 0 1> | <1 -1 0> | 254.4 |
| BN (mp-984) | <0 0 1> | <0 1 0> | 245.5 |
| CdTe (mp-406) | <1 1 0> | <0 1 0> | 122.7 |
| Al (mp-134) | <1 1 0> | <1 0 0> | 250.0 |
| InSb (mp-20012) | <1 1 0> | <0 1 0> | 122.7 |
| ZrO2 (mp-2858) | <0 0 1> | <0 0 1> | 248.2 |
| ZnO (mp-2133) | <1 0 1> | <1 -1 -1> | 177.6 |
| TiO2 (mp-390) | <1 0 1> | <0 1 0> | 122.7 |
| CsI (mp-614603) | <1 1 0> | <1 -1 0> | 254.4 |
| Cu (mp-30) | <1 0 0> | <1 0 0> | 250.0 |
| LiAlO2 (mp-3427) | <0 0 1> | <0 0 1> | 248.2 |
Elasticity
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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Similar Structures
Explanation of dissimilarity measure: Documentation.Calculation Summary
Structure Optimization
Run TypeGGA |
Energy Cutoff520 eV |
# of K-points4 |
U Values-- |
PseudopotentialsVASP PAW: Sr_sv Li_sv La Nb_pv O |
Final Energy/Atom-6.9131 eV |
Corrected Energy-676.6323 eV
-676.6323 eV = -642.9224 eV (uncorrected energy) - 33.7099 eV (MP Anion Correction)
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Detailed input parameters and outputs for all calculations
Submitted by
User remarks:
- ordering of disordered crystal
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)