Superconductors

Iron-Based Superconductors

Iron pnictides and chalcogenides (LaFeAsO, FeSe) discovered in 2008 — the second high-Tc family. Their multiband physics and high critical fields suit high-field magnet wire.

At a glance

Class Statistics

Compounds Tracked
5,953
Multi-Source DFT
230
With Synthesis Routes
0
Avg. Agreement
1.00 / 1.00
Overview

What are Iron-Based Superconductors?

Iron-based superconductors (IBS) represent a transformative class of materials that emerged in 2008, marking the second major family of high-temperature superconductors after the cuprates. Chemically, these materials are primarily composed of iron-pnictide or iron-chalcogenide layers, often interleaved with spacer layers such as rare-earth oxides or alkali metals. The fundamental structure typically features iron atoms arranged in a square lattice, coordinated by pnictogen or chalcogen atoms in a tetrahedral geometry. What makes IBS particularly compelling to the condensed matter community is their complex multiband electronic structure, where multiple charge carriers contribute to the superconducting state. This stands in contrast to the single-band behavior often associated with other systems. Furthermore, these materials exhibit high critical magnetic fields and relatively low anisotropy, which makes them highly attractive for practical engineering applications. Because they can maintain superconductivity under intense magnetic environments, they are considered prime candidates for the development of next-generation high-field magnet wires and power transmission infrastructure. Notable members of this family include the '1111' type, such as LaFeAsO, which first demonstrated the potential for high transition temperatures, and the '11' type, represented by FeSe, which is valued for its structural simplicity and unique electronic properties. As researchers continue to tune their chemical composition through doping or pressure, iron-based superconductors remain at the forefront of efforts to understand the mechanisms of unconventional superconductivity and to push the boundaries of superconducting technology in industrial settings.

Members

Top Iron-Based Superconductors

Ranked by data richness — literature synthesis coverage, multi-source DFT corroboration, and patent activity.

FormulaBand GapBest EAH (eV/atom)StabilityDFT SourcesRecipes
FeSeMetallic / not reported0.0000On hull (stable)40
FeSe20.02–0.37 eV0.0000On hull (stable)20
FeTe20.08 eV0.0000On hull (stable)20
As4Fe20.28 eV0.0000On hull (stable)20
FeAs20.28 eV0.0000On hull (stable)20
FeAsS0.74 eV0.0000On hull (stable)20
As4Fe4S40.74 eV0.0000On hull (stable)20
FeAsO41.30–1.56 eV0.0000On hull (stable)20
Fe2Te40.08 eV0.0000On hull (stable)20
ZrFeSe0.09 eV0.3633Above hull20
AsFeO22.53 eV0.0978Metastable10
FeSeZr0.09 eV0.3633Above hull10
Fe4Se80.02–0.37 eV0.0000On hull (stable)20
Fe4Te80.08 eV0.0000On hull (stable)20
FeTeMetallic / not reported0.0765Metastable20
As8Fe40.28 eV0.0000On hull (stable)20
FeAs2O70.34 eV0.1013Above hull20
Fe4As2O110.73–0.99 eV0.0432Metastable20
Fe4P4Se40.19 eV0.0742Metastable20
ZrFeTe1.16 eV0.0666Metastable20
FeTeAs0.68 eV0.0000On hull (stable)20
TiFeSe0.86 eV0.1960Above hull20
Fe3Se4Metallic / not reported0.0795Metastable40
Fe4Sb4Se40.62 eV0.0000On hull (stable)20
Fe4Sb4Te40.30 eV0.0000On hull (stable)20
As4Fe4Te40.68 eV0.0000On hull (stable)20
As6Fe30.28 eV0.0000On hull (stable)20
Cl14Fe2Se21.32 eV0.0000On hull (stable)20
Cl14Fe2Te21.26 eV0.0000On hull (stable)20
Fe8O20Te41.89 eV0.0256Metastable20
FeSbSe0.62 eV0.0000On hull (stable)20
Fe1Se2V10.06 eV0.0535Metastable10
Fe2Se40.02–0.37 eV0.0000On hull (stable)10
Fe1Se1Zr10.09 eV0.3633Above hull10
As4Fe4Metallic / not reported0.0000On hull (stable)30
As2Fe2La2O21.29 eV0.1730Above hull10
F4Fe4O12Se41.43 eV0.0000On hull (stable)10
Fe2O6Se20.32–0.68 eV0.0828Metastable10
As2Fe2O81.30–1.56 eV0.0000On hull (stable)10
As4Fe4O161.30–1.56 eV0.0000On hull (stable)10
As6Fe6O241.30–1.56 eV0.0000On hull (stable)10
As2Fe10.28 eV0.0000On hull (stable)10
Fe1O3Se10.32–0.68 eV0.0828Metastable10
Fe1Se20.02–0.37 eV0.0000On hull (stable)10
As4Fe4O82.53 eV0.0978Metastable10
F4Fe4O12Te41.50 eV0.0000On hull (stable)10
Fe4O20Te60.40 eV0.2262Above hull10
Fe4Se4Zr40.09 eV0.3633Above hull10
FeTeO3F1.50 eV0.0000On hull (stable)10
MgFeAs2O71.59–2.10 eV0.0066Near hull (likely stable)10
Reference

Frequently Asked Questions

How many iron-based superconductors are in the database?
5,953 iron-based superconductors are tracked, of which 230 have multi-source DFT validation and 0 have documented synthesis routes.
What is the most data-rich iron-based superconductor?
FeSe is the most thoroughly characterized, with 174 reported structures.
Which iron-based superconductor has the widest band gap?
Among the top compounds, AsFeO2 has the widest reported DFT band gap (2.53 eV).
How do iron-based superconductors differ from cuprates?
While both are unconventional superconductors, iron-based materials feature a multi-orbital electronic structure and iron-based layers, whereas cuprates are based on copper-oxide planes and typically exhibit stronger electronic correlations.
Why are these materials useful for high-field magnets?
They possess high upper critical fields and relatively low anisotropy, meaning they can remain superconducting even when subjected to very strong magnetic fields, which is essential for magnet wire performance.
What role does doping play in these materials?
Doping is used to introduce charge carriers into the iron-based layers, which suppresses magnetic order and promotes the emergence of the superconducting state.
Are iron-based superconductors difficult to manufacture?
Manufacturing involves complex synthesis techniques like thin-film deposition or powder-in-tube processing, and managing the chemical sensitivity of the materials remains a key challenge for large-scale production.
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