# Multi-component order parameter superconductivity of Sr$_2$RuO$_4$   revealed by topological junctions

**Authors:** M. S. Anwar, R. Ishiguro, T. Nakamura, M. Yakabe, S. Yonezawa, H., Takayanagi, and Y. Maeno

arXiv: 1703.01814 · 2017-06-21

## TL;DR

This study uses topological Nb/Ru/Sr$_2$RuO$_4$ junctions to investigate the multi-component order parameter of Sr$_2$RuO$_4$, revealing distinct behaviors between the 1.5-K chiral p-wave phase and the 3-K phase.

## Contribution

It demonstrates the use of topological junctions to differentiate between multi-component and single-component superconducting phases in Sr$_2$RuO$_4$.

## Key findings

- Large noise in 1.5-K phase disappears in 3-K phase
- Chiral domain-wall motion explains junction behavior differences
- Confirms multi-component order parameter in 1.5-K phase

## Abstract

Single crystals of the Sr$_2$RuO$_4$-Ru eutectic system are known to exhibit enhanced superconductivity at 3~K, in addition to the bulk superconductivity of Sr$_2$RuO$_4$ at 1.5~K. The 1.5-K phase is believed to be a spin-triplet, chiral $p$-wave state with the multi-component order parameter, giving rise to chiral domain structure. In contrast, the 3-K phase is attributable to enhanced superconductivity of Sr$_2$RuO$_4$ in the strained interface region between Ru inclusion of a few to tens of micrometers in size and the surrounding Sr$_2$RuO$_4$. We investigate the dynamic behavior of a topological junction, where a superconductor is surrounded by another superconductor. Specifically, we fabricated Nb/Ru/Sr$_2$RuO$_4$ topological superconducting junctions, in which the difference in phase winding between the $s$-wave superconductivity in Ru micro-islands induced from Nb and the superconductivity of Sr$_2$RuO$_4$ mainly governs the junction behavior. Comparative results of the asymmetry, hysteresis and noise in junctions with different sizes, shapes, and configurations of Ru inclusions are explained by the chiral domain-wall motion in these topological junctions. Furthermore, a striking difference between the 1.5-K and 3-K phases is clearly revealed: the large noise in the 1.5-K phase sharply disappears in the 3-K phase. These results confirm the multi-component order-parameter superconductivity of the bulk Sr$_2$RuO$_4$, consistent with the chiral $p$-wave state, and the proposed non-chiral single-component superconductivity of the 3-K phase.

## Full text

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## Figures

9 figures with captions in the complete paper: https://tomesphere.com/paper/1703.01814/full.md

## References

40 references — full list in the complete paper: https://tomesphere.com/paper/1703.01814/full.md

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Source: https://tomesphere.com/paper/1703.01814