material
Dy6Ti4Al43
ID:
mp-567159
DOI:
10.17188/1273731
Final Magnetic Moment0.410 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-0.340 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. |
Density4.08 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToStable |
Band Gap0.000 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 MauguinP63/mcm [193] |
Hall-P 6c 2 |
Point Group6/mmm |
Crystal Systemhexagonal |
Electronic Structure
Band Structure and Density of States
X-Ray Diffraction
-
Select radiation source:
- 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%)
X-Ray Absorption Spectra
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Download FEFF Input parameters.
Substrates
Reference for minimal coincident interface area (MCIA) and elastic energy:substrate orientation:
| substrate material | substrate orientation | film orientation | MCIA† [Å2] |
|---|---|---|---|
| CdS (mp-672) | <0 0 1> | <0 0 1> | 106.0 |
| Mg (mp-153) | <0 0 1> | <0 0 1> | 106.0 |
| WS2 (mp-224) | <0 0 1> | <0 0 1> | 106.0 |
| ZrO2 (mp-2858) | <0 1 0> | <1 0 0> | 197.9 |
| YAlO3 (mp-3792) | <1 0 1> | <1 0 0> | 197.9 |
| SrTiO3 (mp-4651) | <1 0 1> | <0 0 1> | 106.0 |
| Bi2Se3 (mp-541837) | <0 0 1> | <0 0 1> | 106.0 |
| MoS2 (mp-1434) | <0 0 1> | <0 0 1> | 106.0 |
| NdGaO3 (mp-3196) | <0 1 1> | <0 0 1> | 106.0 |
| CsI (mp-614603) | <1 1 1> | <0 0 1> | 106.0 |
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-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Dy_3 Ti_pv Al |
Final Energy/Atom-4.4966 eV |
Corrected Energy-476.6423 eV
-476.6423 eV = -476.6423 eV (uncorrected energy)
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Detailed input parameters and outputs for all calculations
ICSD IDs
- 150119
Submitted by
User remarks:
- Dysprosium titanium aluminide (6/4/43)
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)