Pb108Te108
Pb108Te108 has a DFT band gap of 0.10–0.81 eV across 12 reported structures in 5 space groups; its lowest-energy polymorph is cubic (Fm-3m (No. 225)). Cross-validated across 3 computational databases.
At a glance
Key Properties
Cross-validated computational properties for Pb108Te108, aggregated across 3 databases.
Band GapEnergy needed to move an electron from the valence band to the conduction band. Lower or zero values tend to behave more metallic; larger gaps are more insulating or semiconducting.
0.10–0.81 eV
Range across DFT structures
Energy Above HullThermodynamic distance from the most stable set of competing phases. 0 eV/atom is on the convex hull; small positive values may still be experimentally accessible.
0.000 eV/atom
Best (lowest) across sources
StabilityA plain-language summary of the best reported energy-above-hull result. It reflects whether the lowest-energy structure is on, near, or far from the stability hull.
On hull (stable)
1 DFT source
StructuresCount of reported calculated crystal structures for this formula, including alternate polymorphs, source databases, and observed space groups.
12
3 databases, 5 space groups
Crystallography
Reported Structures
Lowest-energy structures reported for Pb108Te108, ranked by energy above hull.
| Space GroupSymmetry classification of the crystal arrangement. The number is the international space-group index. | Crystal SystemBroad lattice family, such as cubic, tetragonal, monoclinic, or triclinic, derived from unit-cell symmetry. | Band Gap (eV)Electronic gap calculated for this specific reported structure, measured in electronvolts. | E above hull (eV/atom)Thermodynamic distance from the convex hull for this structure, normalized per atom. Lower is generally more stable. | E/atom (eV)Computed total energy normalized per atom. Use energy above hull, not this value alone, when comparing stability. | Density (g/cm³)Mass per relaxed crystal volume, reported in grams per cubic centimeter. |
|---|---|---|---|---|---|
| Fm-3m (No. 225) | cubic | 0.81 | 0.0000 | -41.355 | 7.94 |
| P63/mmc (No. 194) | hexagonal | 0.10 | 0.0356 | -41.319 | 7.71 |
| Pnma (No. 62) | orthorhombic | 0.72 | 0.0549 | -41.300 | 7.96 |
| Pnma (No. 62) | orthorhombic | 0.80 | 0.0555 | -41.300 | 7.47 |
| Pm-3m (No. 221) | cubic | 0.00 | 0.2279 | -41.127 | 8.67 |
| — | — | — | — | — | — |
| No. 0 | unknown | — | — | — | 2.07 |
| No. 0 | unknown | — | — | — | 2.18 |
| No. 0 | unknown | — | — | — | 2.08 |
| No. 0 | unknown | — | — | — | 2.07 |
| No. 0 | unknown | — | — | — | 2.05 |
| No. 0 | unknown | — | — | — | 2.06 |
Reference
Frequently Asked Questions
Common questions about Pb108Te108, answered from cross-validated data.
What is the band gap of Pb108Te108?
Pb108Te108 has a DFT-computed band gap of 0.10–0.81 eV across 12 reported structures.
More questions
Is Pb108Te108 a metal, semiconductor, or insulator?
With a band gap up to 0.81 eV it is a semiconductor.
Is Pb108Te108 thermodynamically stable?
Yes — Pb108Te108 sits on the convex hull (energy above hull 0 eV/atom), i.e. on hull (stable).
What is the crystal structure of Pb108Te108?
The lowest-energy reported polymorph of Pb108Te108 is cubic symmetry, space group Fm-3m (No. 225).
What is the density of Pb108Te108?
The computed density of the ground-state structure of Pb108Te108 is 7.94 g/cm³.
How many polymorphs of Pb108Te108 are known?
12 structures of Pb108Te108 are reported across 3 databases, spanning 5 distinct space groups.
What elements does Pb108Te108 contain?
Pb108Te108 contains Pb and Te (2 elements).
Where does the data for Pb108Te108 come from?
Pb108Te108 data is cross-referenced from materials_project, nomad, cod.
Explore
Related Compounds
Other Lead Chalcogenide Thermoelectrics in the database.
Data sources & attribution
- materials_project — Data from the Materials Project. Cite: Jain et al., APL Materials 1, 011002 (2013).
- nomad — Data from NOMAD. Cite: Draxl & Scheffler, J. Phys. Mater. 2, 036001 (2019).
- cod — Data from the Crystallography Open Database. Cite: Grazulis et al., Nucleic Acids Res. 40, D420 (2012).
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