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Simon John Bending

Publications and source records attributed to Simon John Bending.

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Breakdown of the critical state in the ferromagnetic superconductor EuFe$_2$(As$_{1-x}$P$_x$)$_2$

There are very few materials in which ferromagnetism coexists with superconductivity due to the destructive effect of the magnetic exchange field on singlet Cooper pairs. The iron-based superconductor EuFe$_2$(As$_{1-x}$P$_x$)$_2$ is therefore unique in exhibiting robust superconductivity with a maximum critical temperature of 25 K and long-range ferromagnetism below $T_\mathrm{FM}\approx19$ K. Here we report a spatially-resolved study of the irreversible magnetisation in this system that reveals a variety of novel behaviours that are strongly linked with underlying ferromagnetic domain structures. In the superconducting-only state, hysteretic magnetisation due to irreversible vortex motion is consistent with typical weak vortex-pinning behaviour. Just below $T_\mathrm{FM}$, very narrowly-spaced stripe domains give rise to highly erratic and irreproducible fluctuations in the irreversible magnetisation that we attribute to the dynamics of multi-vortex clusters stabilised by the formation of vortex polarons. In contrast, at lower temperatures, ferromagnetic domains become wider and saturated with spontaneously nucleated vortices and antivortices, leading to a smoother but unconventional evolution of the irreversible state. This observation suggests that the penetrating flux front is roughened by the presence of the magnetic domains in this regime, presenting a clear departure from standard critical state models. Our findings indicate that the mechanism governing irreversibility is strongly influenced by the precise nature of the underlying ferromagnetic domains, being very sensitive to the specific material parameters of EuFe$_2$(As$_{1-x}$P$_x$)$_2$. We consider the possible microscopic origins of these effects, and suggest further ways to explore novel vortex-domain magnetic behaviours.

cond-mat.supr-con

Magnetically-controlled Vortex Dynamics in a Ferromagnetic Superconductor

Ferromagnetic superconductors are exceptionally rare because the strong ferromagnetic exchange field usually destroys singlet superconductivity. EuFe$_2$(As$_{1-x}$P$_x$)$_2$, an iron-based superconductor with a maximum critical temperature of 25 K, uniquely exhibits full coexistence with ferromagnetic order below $T_\mathrm{FM}$ $\simeq$ $19$ K. The interplay leads to narrowing of ferromagnetic domains at higher temperatures and spontaneous nucleation of vortices/antivortices at lower temperatures. Here we demonstrate how the underlying magnetic structure controls the superconducting vortex dynamics in applied magnetic fields. Just below $T_\mathrm{FM}$ we observe a pronounced peak in the creep activation energy, and magnetic force microscopy measurements reveal the presence of very closely-spaced ($w\ll λ$) vortex clusters. We attribute these observations to the formation of vortex polarons for which we present a theoretical description. In contrast, we link strong magnetic irreversibility at low temperatures to a critical current governed by giant flux creep over an activation barrier for vortex-antivortex annihilation near domain walls. Our work suggests new routes for the magnetic enhancement of vortex pinning with important applications in high-current conductors.

cond-mat.supr-con