# Synthesis, crystal structure and superconductivity in   Rb$Ln_2$Fe$_4$As$_4$O$_2$ ($Ln$ = Sm, Tb, Dy and Ho)

**Authors:** Zhi-Cheng Wang, Chao-Yang He, Si-Qi Wu, Zhang-Tu Tang, Yi Liu, and, Guang-Han Cao

arXiv: 1704.01075 · 2017-04-05

## TL;DR

This study reports the synthesis and structural analysis of new Rb$Ln_2$Fe$_4$As$_4$O$_2$ superconductors with $Ln$ = Sm, Tb, Dy, Ho, revealing their phase formation, intrinsic doping, and superconducting transition temperatures around 34-36 K.

## Contribution

It introduces a new class of iron-based superconductors formed by intergrowth of RbFe$_2$As$_2$ and $Ln$FeAsO, highlighting the importance of lattice matching and interlayer coupling for superconductivity.

## Key findings

- Superconductivity observed at 33.8-35.8 K.
- Structural intergrowth causes intrinsic doping of 0.25 holes/Fe.
- Interlayer coupling influences $T_c$ optimization.

## Abstract

We have synthesized four iron-based oxyarsenide superconductors Rb$Ln_2$Fe$_4$As$_4$O$_2$ ($Ln$ = Sm, Tb, Dy and Ho) resulting from the intergrowth of RbFe$_2$As$_2$ and $Ln$FeAsO. It is found that the lattice match between RbFe$_2$As$_2$ and $Ln$FeAsO is crucial for the phase formation. The structural intergrowth leads to double asymmetric Fe$_2$As$_2$ layers that are separated by insulating $Ln_2$O$_2$ slabs. Consequently, the materials are intrinsically doped at a level of 0.25 holes/Fe-atom and, bulk superconductivity emerges at $T_\mathrm{c}$ = 35.8, 34.7, 34.3 and 33.8 K, respectively, for $Ln$ = Sm, Tb, Dy and Ho. Investigation on the correlation between crystal structure and $T_\mathrm{c}$ suggests that interlayer couplings may play an additional role for optimization of superconductivity.

## Full text

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## Figures

9 figures with captions in the complete paper: https://tomesphere.com/paper/1704.01075/full.md

## References

33 references — full list in the complete paper: https://tomesphere.com/paper/1704.01075/full.md

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Source: https://tomesphere.com/paper/1704.01075