
Deliberately adding excess iron overturns traditional impurity assumptions, offering a tunable platform to boost critical temperatures and explore superconductivity‑magnetism coupling, which could accelerate the development of loss‑less power transmission technologies.
Iron‑based chalcogenides have long been a focal point for high‑temperature superconductivity research, yet pristine FeSe stalls at a modest 8.5 K. Efforts to raise this ceiling have centered on chemical intercalation, strain engineering, and substrate effects, each providing incremental gains but often introducing structural instability. The new Fe₁.₁₁Se crystals break this pattern by embracing, rather than eliminating, interstitial iron—a strategy that redefines impurity management and opens a broader compositional landscape for superconducting design.
The breakthrough hinges on a two‑step hydrothermal ion‑exchange followed by selective de‑intercalation, which precisely inserts 11 % extra Fe into the lattice while preserving the LiFeAs‑type framework. Structural probes confirm expanded interlayer spacing and random occupation of the 2c site, correlating with a dramatic Tc onset of 30.4 K. When subjected to pressures between 2 and 2.6 GPa, the material exhibits a V‑shaped Tc trajectory, first dipping then rebounding, a hallmark of competing electronic orders. Concurrently, spectroscopic signatures hint at pressure‑induced magnetic ordering, suggesting that magnetism and superconductivity are more intimately linked than previously thought.
For the energy sector, such pressure‑tunable, higher‑Tc superconductors could eventually enable lossless power grids and compact magnetic devices, provided scalability challenges are addressed. The hydrothermal route, while promising for laboratory‑scale synthesis, must be adapted for bulk production and long‑term stability. Nonetheless, the study establishes a viable blueprint: leveraging non‑equilibrium chemistry to engineer interstitial defects that enhance performance. Future work will likely explore similar strategies across other layered superconductors, accelerating the march toward practical, room‑temperature superconductivity.
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