Be4Cl12Te14

Be4Cl12Te14 is a thermodynamically stable semiconducting compound composed of beryllium, chlorine, and tellurium.

BeClTe
Crystal structure of Be4Cl12Te14 (orthorhombic, Pnnm (No. 58))
Ground-state structure · Materials Project
Overview

About Be4Cl12Te14

Be4Cl12Te14 is a complex inorganic compound characterized by its semiconducting electronic nature. As a thermodynamically stable phase residing on the convex hull, it represents a robust structural arrangement of beryllium, chlorine, and tellurium atoms. Its stability suggests potential for integration into specialized electronic or optoelectronic frameworks where reliable material behavior is required. The material has garnered interest in structural databases, reflecting its unique crystallographic profile and the ongoing efforts to map its potential utility. Its existence as a stable phase makes it a compelling subject for researchers investigating the interplay between chalcogenide chemistry and light-element coordination.

At a glance

Key Properties

Cross-validated computational properties for Be4Cl12Te14, aggregated across 3 databases.

Band Gap

1.28 eV
Range across DFT structures

Energy Above Hull

0.001 eV/atom
Best (lowest) across sources

Stability

On hull (stable)
2 DFT sources

Structures

6
3 databases, 1 space group
Crystallography

Reported Structures

Lowest-energy structures reported for Be4Cl12Te14, ranked by energy above hull.

Space GroupCrystal SystemBand Gap (eV)E above hull (eV/atom)E/atom (eV)Density (g/cm³)
Pnnm (No. 58)orthorhombic1.280.0006-3.6264.07
3.86
3.86
Pnnm (No. 58)
3.86
3.86
Uses

Applications

Where Be4Cl12Te14 is used.

Materials science researchSemiconductor developmentSolid-state chemistry studies
Reference

Frequently Asked Questions

Common questions about Be4Cl12Te14, answered from cross-validated data.

What is Be4Cl12Te14?

Be4Cl12Te14 is a thermodynamically stable semiconducting compound composed of beryllium, chlorine, and tellurium.

More questions
What is Be4Cl12Te14 used for?
Be4Cl12Te14 is used in materials science research, semiconductor development, and solid-state chemistry studies.
What is the band gap of Be4Cl12Te14?
Be4Cl12Te14 has a DFT-computed band gap of 1.28 eV across 6 reported structures.
Is Be4Cl12Te14 a metal, semiconductor, or insulator?
With a band gap up to 1.28 eV it is a semiconductor.
Is Be4Cl12Te14 thermodynamically stable?
Yes — Be4Cl12Te14 sits on the convex hull (energy above hull 0 eV/atom), i.e. on hull (stable).
What is the crystal structure of Be4Cl12Te14?
The lowest-energy reported polymorph of Be4Cl12Te14 is orthorhombic symmetry, space group Pnnm (No. 58).
What is the density of Be4Cl12Te14?
The computed density of the ground-state structure of Be4Cl12Te14 is 4.07 g/cm³.
How many polymorphs of Be4Cl12Te14 are known?
6 structures of Be4Cl12Te14 are reported across 3 databases, spanning 1 distinct space group.
What elements does Be4Cl12Te14 contain?
Be4Cl12Te14 contains Be, Cl, and Te (3 elements).
Where does the data for Be4Cl12Te14 come from?
Be4Cl12Te14 data is cross-referenced from materials_project, omat24, aflow.
Comparison

How It Compares

As a unique inorganic phase, Be4Cl12Te14 stands as a distinct structural entity within the broader landscape of complex beryllium-based halides and tellurides. While it currently lacks direct structural siblings in this specific classification, its stability and semiconducting nature position it as a benchmark for exploring multi-component systems that balance high-electronegativity halogens with heavy, semi-metallic elements.

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).
  • aflow — Data from AFLOW. Cite: Curtarolo et al., Comp. Mater. Sci. 58, 218 (2012).

Analyze Be4Cl12Te14 in the Lattice Graph platform

Polymorph comparison, confidence scoring, supply-chain risk, and patent monitoring — across 53 integrated data sources.

Explore the Platform →