Li10BrN3
Li10BrN3 is a thermodynamically stable, semiconducting inorganic compound composed of lithium, bromine, and nitrogen.
About Li10BrN3
Li10BrN3 is a distinct inorganic compound characterized by its semiconducting electronic nature. As a material that resides on the convex hull, it exhibits notable thermodynamic stability, making it a compelling subject for researchers investigating lithium-based solid-state chemistry.
Its structural profile is well-documented, with multiple reported configurations across major databases. This data richness supports its role as a candidate for specialized applications where stable, semiconducting lithium-nitrogen-bromine frameworks are required.
Key Properties
Cross-validated computational properties for Li10BrN3, 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.
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.
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.
StructuresCount of reported calculated crystal structures for this formula, including alternate polymorphs, source databases, and observed space groups.
Reported Structures
Lowest-energy structures reported for Li10BrN3, 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. |
|---|---|---|---|---|---|
| P-6m2 (No. 187) | hexagonal | 1.37 | 0.0000 | -3.930 | 1.76 |
| P-6m2 (No. 187) | Hexagonal | — | — | — | 1.71 |
| P-6m2 (No. 187) | Hexagonal | — | — | — | 1.74 |
| P-6m2 (No. 187) | Hexagonal | — | — | — | 1.76 |
| P-6m2 (No. 187) | — | — | — | — | — |
Applications
Where Li10BrN3 is used.
Frequently Asked Questions
Common questions about Li10BrN3, answered from cross-validated data.
What is Li10BrN3?
Li10BrN3 is a thermodynamically stable, semiconducting inorganic compound composed of lithium, bromine, and nitrogen.
What is Li10BrN3 used for?
What is the band gap of Li10BrN3?
Is Li10BrN3 a metal, semiconductor, or insulator?
Is Li10BrN3 thermodynamically stable?
What is the crystal structure of Li10BrN3?
What is the density of Li10BrN3?
How many polymorphs of Li10BrN3 are known?
What elements does Li10BrN3 contain?
Where does the data for Li10BrN3 come from?
How It Compares
As a unique entry in its chemical space, Li10BrN3 serves as a foundational example of how lithium, nitrogen, and bromine can organize into a thermodynamically favored, semiconducting architecture.
Data sources & attribution
- materials_project — Data from the Materials Project. Cite: Jain et al., APL Materials 1, 011002 (2013).
- mpaloe — Data from mpaloe.
- jarvis — Data from JARVIS (NIST). Cite: Choudhary et al., npj Comp. Mater. 6, 173 (2020).
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