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Giant superconducting fluctuations in the compensated semimetal FeSe at the BCS–BEC crossover

机译:BCS–BEC交叉处的补偿半金属FeSe的超导大波动

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摘要

The physics of the crossover between weak-coupling Bardeen–Cooper–Schrieffer (BCS) and strong-coupling Bose–Einstein condensate (BEC) limits gives a unified framework of quantum-bound (superfluid) states of interacting fermions. This crossover has been studied in the ultracold atomic systems, but is extremely difficult to be realized for electrons in solids. Recently, the superconducting semimetal FeSe with a transition temperature Tc=8.5 K has been found to be deep inside the BCS–BEC crossover regime. Here we report experimental signatures of preformed Cooper pairing in FeSe, whose energy scale is comparable to the Fermi energies. In stark contrast to usual superconductors, large non-linear diamagnetism by far exceeding the standard Gaussian superconducting fluctuations is observed below T*∼20 K, providing thermodynamic evidence for prevailing phase fluctuations of superconductivity. Nuclear magnetic resonance and transport data give evidence of pseudogap formation at ∼T*. The multiband superconductivity along with electron–hole compensation in FeSe may highlight a novel aspect of the BCS–BEC crossover physics.
机译:弱耦合的Bardeen-Cooper-Schrieffer(BCS)和强耦合的Bose-Einstein凝聚物(BEC)限度之间的交越物理给出了相互作用的费米子的量子束缚(超流体)状态的统一框架。已经在超冷原子系统中研究了这种交叉,但是对于固体中的电子而言,实现这种交叉极为困难。最近,已经发现过渡温度为Tc = 8.5 K的超导半金属FeSe位于BCS-BEC交叉区深处。在这里,我们报告在FeSe中预形成库珀配对的实验特征,其能量规模可与费米能量相媲美。与通常的超导体形成鲜明对比的是,在T *〜20 K以下观察到大的非线性反磁性远远超过了标准的高斯超导波动,为超导的主要相位波动提供了热力学证据。核磁共振和传输数据提供了在〜T *处伪间隙形成的证据。 FeSe中的多带超导性和电子-空穴补偿可能突出了BCS-BEC交叉物理学的一个新方面。

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