A BCS-like gap in the superconductor SmFeAsO0.85F0.15

A BCS-like gap in the superconductor SmFeAsO0.85F0.15
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超导体 SmFeAsO0.85F0.15 中类似 BCS 的间隙

DOI:
10.1038/nature07081
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发表时间:
2008-05
期刊:
影响因子:
64.8
通讯作者:
Liu, R. H.
Liu, R. H.
中科院分区:
综合性期刊1区
文献类型:
--
作者:
Chien, C. L.;Tesanovic, Z.;Chen, T. Y.;Chen, X. H.;Liu, R. H.

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自从20年前在高转变温度(high-Tc)铜氧化物中发现超导性以来,人们已经牢固地确立了CuO 2平面对于超导性是必不可少的,并且产生了许多其他非常不寻常的性质。最近发现了一个新的超导体家族,其一般组成为LaFeAsO 1-xFx,超导能隙(其大小、结构和温度依赖性)与配对密切相关。本文报道了用Andreev谱测量的超导体SmFeAsO_(0.85)F_(0.15)(Tc = 42 K)中的单能隙。差距值2Δ= 13.34 ± 0.3 meV,得到2Δ/kBTc= 3.68(其中kB是玻尔兹曼常数),接近巴丁-库珀-施里弗(BCS)预测的3.53。差距随温度的升高而减小,在T_c处消失,这与BCS理论的预言一致,但与氧化铜超导体中的赝间隙行为有很大的不同。我们的研究结果清楚地表明,nodeless间隙序参数,这是几乎各向同性的费米表面的不同部分的大小,并不兼容的模型,涉及反铁磁波动,强相关性,thet-J模型等,最初设计的高Tc铜氧化物。
Since the discovery of superconductivity in the high-transition-temperature (high-Tc) copper oxides two decades ago, it has been firmly established that the CuO2plane is essential for superconductivity and gives rise to a host of other very unusual properties. A new family of superconductors with the general composition of LaFeAsO1-xFxhas recently been discovered,,,,,,,and the conspicuous lack of the CuO2planes raises the tantalizing question of a different pairing mechanism in these oxypnictides. The superconducting gap (its magnitude, structure, and temperature dependence) is intimately related to pairing. Here we report the observation of a single gap in the superconductor SmFeAsO0.85F0.15withTc= 42 K as measured by Andreev spectroscopy. The gap value of 2Δ= 13.34 ± 0.3 meV gives 2Δ/kBTc= 3.68 (wherekBis the Boltzmann constant), close to the Bardeen–Cooper–Schrieffer (BCS) prediction of 3.53. The gap decreases with temperature and vanishes atTcin a manner consistent with the BCS prediction, but dramatically different from that of the pseudogap behaviour in the copper oxide superconductors. Our results clearly indicate a nodeless gap order parameter, which is nearly isotropic in size across different sections of the Fermi surface, and are not compatible with models involving antiferromagnetic fluctuations, strong correlations, thet-Jmodel, and the like, originally designed for the high-Tccopper oxides.
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