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arxiv: 1710.10895 · v2 · pith:D2MQC2E7new · submitted 2017-10-30 · ❄️ cond-mat.supr-con · cond-mat.mtrl-sci· cond-mat.str-el

RbEu(Fe_(1-x)Ni_x)₄As₄: From a ferromagnetic superconductor to a superconducting ferromagnet

classification ❄️ cond-mat.supr-con cond-mat.mtrl-scicond-mat.str-el
keywords mathrmsuperconductingferromagneticferromagnetrbeurbeufesuperconductoradditionally
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The intrinsically hole-doped RbEuFe$_4$As$_4$ exhibits bulk superconductivity at $T_{\mathrm{sc}}=36.5$ K and ferromagnetic ordering in the Eu sublattice at $T_\mathrm{m}=15$ K. Here we present a hole-compensation study by introducing extra itinerant electrons via a Ni substitution in the ferromagnetic superconductor RbEuFe$_4$As$_4$ with $T_{\mathrm{sc}}>T_{\mathrm{m}}$. With the Ni doping, $T_{\mathrm{sc}}$ decreases rapidly, and the Eu-spin ferromagnetism and its $T_{\mathrm{m}}$ remain unchanged. Consequently, the system RbEu(Fe$_{1-x}$Ni$_x$)$_4$As$_4$ transforms into a superconducting ferromagnet with $T_{\mathrm{m}}>T_{\mathrm{sc}}$ for $0.07\leq x\leq0.08$. The occurrence of superconducting ferromagnets is attributed to the decoupling between Eu$^{2+}$ spins and superconducting Cooper pairs. The superconducting and magnetic phase diagram is established, which additionally includes a recovered yet suppressed spin-density-wave state.

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