C6Zr6
C6Zr6 has a DFT band gap of 0.48 eV across 13 reported structures in 7 space groups; its lowest-energy polymorph is cubic (Fm-3m (No. 225)). Cross-validated across 5 computational databases.
Overview
Key Properties
Cross-validated computational properties for C6Zr6, aggregated across 5 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.
0.48 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)
3 DFT sources
StructuresCount of reported calculated crystal structures for this formula, including alternate polymorphs, source databases, and observed space groups.
13
5 databases, 7 space groups
Crystallography
Reported Structures
Lowest-energy structures reported for C6Zr6, 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 | 0.00 | 0.0000 | -17.362 | 6.55 |
| P63/mmc (No. 194) | hexagonal | 0.00 | 0.1685 | -17.194 | 6.51 |
| F-43m (No. 216) | cubic | 0.48 | 0.6133 | -16.749 | 5.15 |
| Pm-3m (No. 221) | cubic | 0.00 | 1.2194 | -16.143 | 6.78 |
| — | — | — | — | — | 4.84 |
| — | — | — | — | — | 4.84 |
| No. 0 | unknown | — | — | — | 1.67 |
| P63/mmc (No. 194) | — | — | — | — | — |
| P-3m1 (No. 164) | — | — | — | — | — |
| R-3m (No. 166) | — | — | — | — | — |
| R-3m (No. 166) | — | — | — | — | — |
| No. 0 | unknown | — | — | — | 1.62 |
Reference
Frequently Asked Questions
Common questions about C6Zr6, answered from cross-validated data.
What is the band gap of C6Zr6?
C6Zr6 has a DFT-computed band gap of 0.48 eV across 13 reported structures.
More questions
Is C6Zr6 a metal, semiconductor, or insulator?
With a band gap up to 0.48 eV it is a semiconductor.
Is C6Zr6 thermodynamically stable?
Yes — C6Zr6 sits on the convex hull (energy above hull 0 eV/atom), i.e. on hull (stable).
What is the crystal structure of C6Zr6?
The lowest-energy reported polymorph of C6Zr6 is cubic symmetry, space group Fm-3m (No. 225).
What is the density of C6Zr6?
The computed density of the ground-state structure of C6Zr6 is 6.55 g/cm³.
How many polymorphs of C6Zr6 are known?
13 structures of C6Zr6 are reported across 5 databases, spanning 7 distinct space groups.
What elements does C6Zr6 contain?
C6Zr6 contains C and Zr (2 elements).
Where does the data for C6Zr6 come from?
C6Zr6 data is cross-referenced from materials_project, omat24, cod, aflow, nomad.
Explore
Related Compounds
Other Ultra-High-Temperature Ceramics in the database.
Data sources & attribution
- materials_project — Data from the Materials Project. Cite: Jain et al., APL Materials 1, 011002 (2013).
- omat24 — Data from OMat24 (Meta FAIR). Cite: Barroso-Luque et al., arXiv 2410.12771 (2024).
- cod — Data from the Crystallography Open Database. Cite: Grazulis et al., Nucleic Acids Res. 40, D420 (2012).
- aflow — Data from AFLOW. Cite: Curtarolo et al., Comp. Mater. Sci. 58, 218 (2012).
- nomad — Data from NOMAD. Cite: Draxl & Scheffler, J. Phys. Mater. 2, 036001 (2019).
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