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Enhanced superconducting transition temperature in hyper-interlayer-expanded FeSe despite the suppressed electronic nematic order and spin fluctuations

Matevž Majcen Hrovat, Peter Jeglič, Martin Klanjšek, Takehiro Hatakeda, Takashi Noji, Yoichi Tanabe, Takahiro Urata, Khuong K. Huynh, Yoji Koike, Katsumi Tanigaki, Denis Arčon

DOI 10.1103/PhysRevB.92.094513 · Physical Review B

T1

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Abstract

The superconducting critical temperature, Tc, of FeSe can be dramatically enhanced by intercalation of a molecular spacer layer. Here we report on a Se77,Li7, and H1 nuclear magnetic resonance (NMR) study of the powdered hyper-interlayer-expanded Lix(C2H8N2)yFe2−zSe2 with a nearly optimal Tc=45 K. The absence of any shift in the Li7 and H1 NMR spectra indicates a complete decoupling of interlayer units from the conduction electrons in FeSe layers, whereas nearly temperature-independent Li7 and H1 spin-lattice relaxation rates are consistent with the non-negligible concentration of Fe impurities present in the insulating interlayer space. On the other hand, the strong temperature dependence of Se77 NMR shift and spin-lattice relaxation rate, 1/77T1, is attributed to the holelike bands close to the Fermi energy. 1/77T1 shows no additional anisotropy that would account for the onset of electronic nematic order down to Tc. Similarly, no enhancement in 1/77T1 due to the spin fluctuations could be found in the normal state. Yet, a characteristic power-law dependence 1/77T1∝T4.5 still complies with the Cooper pairing mediated by spin fluctuations.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Lix(C2H8N2)yFe2-zSe2

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45Pressure unresolvedonset
FeSe

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8Pressure unresolvedonset
FeSe

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377 GPaunknown

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