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首页> 外文期刊>Physical review letters >Long-Range Proximity Effect for Opposite-Spin Pairs in Superconductor-Ferromagnet Heterostructures Under Nonequilibrium Quasiparticle Distribution
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Long-Range Proximity Effect for Opposite-Spin Pairs in Superconductor-Ferromagnet Heterostructures Under Nonequilibrium Quasiparticle Distribution

机译:非平衡准粒子分布下超导体-铁磁体异质结构中相反自旋对的远距离效应

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摘要

By now it is known that in a singlet superconductor-ferromagnet (S-F) structure the superconducting correlations carried by opposite-spin pairs penetrate into the ferromagnet over a short distance of the order of magnetic coherence length. The long-range proximity effect (LRPE), taking place on the length scale of the normal metal coherence length, can only be maintained by equal-spin pairs, which can be generated by magnetic inhomogeneities in the system. In this Letter, we have predicted a new type of LRPE, which can take place in S-F heterostructures under nonequilibrium conditions. The superconducting correlations in the F region are generated by opposite-spin Cooper pairs and equal-spin pairs are not involved. The possibility for an opposite-spin pair to penetrate into the ferromagnet over a large distance is provided by creation of the proper nonequilibrium quasiparticle distribution there. This leads to a sharp increase (up to a few orders of magnitude) of the critical Josephson current through a S-F-S junction at some values of the voltage controlling the nonequilibrium distribution in the F interlayer.
机译:到目前为止,已知在单重态超导体-铁磁体(S-F)结构中,由相反自旋对所携带的超导相关在磁相干长度量级的短距离内渗透到铁磁体中。在正常金属相干长度的长度尺度上发生的远距离邻近效应(LRPE),只能由等旋转对来维持,该对可以由系统中的磁不均匀性产生。在这封信中,我们已经预测了一种新型的LRPE,它可以在非平衡条件下发生在S-F异质结构中。 F区域中的超导相关性是由相反自旋的Cooper对产生的,而不包含自旋的对偶。通过在此处创建适当的非平衡准粒子分布,可以使反向旋转对在很长的距离内穿透铁磁体。这导致在控制F中间层中非平衡分布的某些电压值下,通过S-F-S结的约瑟夫森临界电流急剧增加(最多几个数量级)。

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