B2F3

B2F3 is an unstable, semiconducting binary compound of boron and fluorine characterized by a variety of known structural arrangements.

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Crystal structure of B2F3 (monoclinic, P2/c (No. 13))
Ground-state structure · Materials Project
Overview

About B2F3

B2F3 is a binary compound composed of boron and fluorine that exhibits semiconducting electronic properties. Its existence is marked by a diverse range of reported structural configurations, reflecting the complex bonding landscape inherent to boron-fluorine systems.

Due to its position above the thermodynamic hull, B2F3 is considered a metastable or unstable phase under standard conditions. This characteristic makes it a subject of interest for researchers investigating high-energy chemical environments and the fundamental limits of boron-based material stability.

At a glance

Key Properties

Cross-validated computational properties for B2F3, aggregated across 4 databases.

Band Gap

2.43 eV
Range across DFT structures · ground state: wide gap

Energy Above Hull

0.170 eV/atom
Best (lowest) across sources

Stability

Unstable
2 DFT sources

Structures

15
4 databases, 6 space groups
Validation

Cross-Source DFT Agreement

How well independent DFT databases agree on the thermodynamics of B2F3. Tight agreement means computed properties can be trusted without re-running calculations.

Agreement Score

0.00 / 1.00
Trust tier: low

Hull Spread

1.372 eV
EAH spread across sources

Sources Compared

2
materials_project, oqmd

Space Group Consensus

—
Crystallography

Reported Structures

Lowest-energy structures reported for B2F3, ranked by energy above hull.

Space GroupCrystal SystemBand Gap (eV)E above hull (eV/atom)E/atom (eV)Density (g/cm³)
P2/c (No. 13)monoclinic2.430.1695-6.1401.77
——0.001.5413-0.853—
P-1 (No. 2)triclinic———2.89
P-1 (No. 2)triclinic———2.82
P-1 (No. 2)triclinic———4.16
P-1 (No. 2)triclinic———4.16
P-1 (No. 2)triclinic———3.08
C2/m (No. 12)monoclinic———3.09
P-1 (No. 2)triclinic———3.07
Pm (No. 6)monoclinic———2.09
Pm (No. 6)monoclinic———2.37
P2/m (No. 10)monoclinic———3.28
Reference

Frequently Asked Questions

Common questions about B2F3, answered from cross-validated data.

What is B2F3?

B2F3 is an unstable, semiconducting binary compound of boron and fluorine characterized by a variety of known structural arrangements.

More questions
What is the band gap of B2F3?
B2F3 has a DFT-computed band gap of 2.43 eV across 15 reported structures. Standard DFT underestimates band gaps, so the measured gap is typically larger.
Is B2F3 a metal, semiconductor, or insulator?
DFT predicts a band gap of up to 2.43 eV (a semiconductor). Measured gaps are typically larger.
Is B2F3 thermodynamically stable?
B2F3 has a lowest energy above hull of 0.170 eV/atom (unstable).
What is the crystal structure of B2F3?
The reference structure of B2F3 is monoclinic symmetry, space group P2/c (No. 13).
What is the density of B2F3?
The computed density of the ground-state structure of B2F3 is 1.77 g/cm³.
How many polymorphs of B2F3 are known?
15 structures of B2F3 are reported across 4 databases, spanning 6 distinct space groups.
What elements does B2F3 contain?
B2F3 contains B and F (2 elements).
Where does the data for B2F3 come from?
B2F3 data is cross-referenced from materials_project, oqmd, mpaloe, cod.
Comparison

How It Compares

As an unclassified and thermodynamically unstable phase, B2F3 represents a specialized area of study within boron-fluorine chemistry, serving as a case study for identifying metastable structures that do not readily persist in equilibrium.

Data sources & attribution
  • materials_project — Data from the Materials Project (materialsproject.org). Cite: Jain et al., APL Materials 1, 011002 (2013). (CC-BY-4.0)
  • oqmd — Data from the OQMD (oqmd.org). Cite: Saal et al., JOM 65, 1501 (2013); Kirklin et al., npj Comp. Mater. 1, 15010 (2015). (CC-BY-4.0)
  • mpaloe — Data from MP-ALOE. Cite: Kuner et al., npj Comput. Mater. (2025), doi:10.1038/s41524-025-01834-9.
  • cod — Data from the Crystallography Open Database (crystallography.net/cod/). Cite: Grazulis et al., J. Appl. Cryst. 42, 726 (2009). (CC0-1.0)

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