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arxiv: 1102.2783 · v1 · pith:OLSQDIDKnew · submitted 2011-02-14 · ❄️ cond-mat.supr-con · cond-mat.mtrl-sci

Coexistence of superconductivity and antiferromagnetism in single crystals A_(0.8)Fe_(2-y)Se₂ (A= K, Rb, Cs, Tl/K and Tl/Rb): evidence from magnetization and resistivity

classification ❄️ cond-mat.supr-con cond-mat.mtrl-sci
keywords resistivitysusceptibilitytemperaturecrystalssuperconductivitytransitionantiferromagneticantiferromagnetism
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We measure the resistivity and magnetic susceptibility in the temperature range from 5 K to 600 K for the single crystals $A$Fe$_{2-y}$Se$_2$ ($A$ = K$_{0.8}$, Rb$_{0.8}$, Cs$_{0.8}$, Tl$_{0.5}$K$_{0.3}$ and Tl$_{0.4}$Rb$_{0.4}$). A sharp superconducting transition is observed in low temperature resistivity and susceptibility, and susceptibility shows 100% Meissner volume fraction for all crystals, while an antiferromagnetic transition is observed in susceptibility at Neel temperature ($T_N$) as high as 500 K to 540 K depending on A. It indicates the coexistence of superconductivity and antiferromagnetism. A sharp increase in resistivity arises from the structural transition due to Fe vacancy ordering at the temperature slightly higher than $T_{\rm N}$. Occurrence of superconductivity in an antiferromagnetic ordered state with so high $T_{\rm N}$ may suggest new physics in this type of unconventional superconductors.

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