material
Mn2SnC10(ClO5)2
ID:
mp-637617
DOI:
10.17188/1279711
- Structure is highly unstable (calculated energy above hull > 100 meV).
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-0.873 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.534 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. |
Density2.13 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToCO2 + C + SnCl2 + MnCO3 |
Band Gap2.681 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 |
Band Structure
Density of States
sign indicates spin ↑ ↓
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 spectra for every symmetrically equivalent absorption site in the structure.
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] |
|---|---|---|---|
| AlN (mp-661) | <1 1 1> | <0 0 1> | 257.3 |
| Te2W (mp-22693) | <0 0 1> | <1 0 -1> | 176.7 |
| CdS (mp-672) | <1 0 0> | <0 0 1> | 257.3 |
| LiF (mp-1138) | <1 0 0> | <1 0 0> | 198.9 |
| Te2W (mp-22693) | <1 0 1> | <1 0 0> | 198.9 |
| Ag (mp-124) | <1 0 0> | <0 0 1> | 257.3 |
| TeO2 (mp-2125) | <1 1 0> | <1 0 0> | 198.9 |
| SiC (mp-7631) | <0 0 1> | <1 0 0> | 198.9 |
| TiO2 (mp-2657) | <1 1 0> | <0 0 1> | 257.3 |
| LaF3 (mp-905) | <1 1 1> | <1 0 0> | 198.9 |
| Ni (mp-23) | <1 0 0> | <0 0 1> | 257.3 |
| SiC (mp-11714) | <0 0 1> | <1 0 0> | 198.9 |
| SiC (mp-11714) | <1 0 1> | <0 1 1> | 195.0 |
| C (mp-48) | <1 0 1> | <1 0 0> | 198.9 |
| ZnO (mp-2133) | <1 0 1> | <1 0 0> | 198.9 |
| LiAlO2 (mp-3427) | <1 0 0> | <1 0 0> | 198.9 |
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+U |
Energy Cutoff520 eV |
# of K-points3 |
U ValuesMn: 3.9 eV |
PseudopotentialsVASP PAW: Mn_pv Sn_d C Cl O |
Final Energy/Atom-7.1157 eV |
Corrected Energy-753.1082 eV
-753.1082 eV = -711.5698 eV (uncorrected energy) - 28.0916 eV (MP Anion Correction) - 13.4468 eV (MP Advanced Correction)
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Detailed input parameters and outputs for all calculations
ICSD IDs
- 27355
Submitted by
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)