凝聚态物理
超导电性
物理
铁磁性
单重态
三重态
约瑟夫森效应
超电流
自旋(空气动力学)
磁化
库珀对
磁场
量子力学
激发态
热力学
作者
R. S. Keizer,Sebastian T. B. Goennenwein,T. M. Klapwijk,Guo‐Xing Miao,Gang Xiao,Arunava Gupta
出处
期刊:Nature
[Nature Portfolio]
日期:2006-02-01
卷期号:439 (7078): 825-827
被引量:676
摘要
In general, conventional superconductivity should not occur in a ferromagnet, though it has been seen in iron under pressure. Moreover, theory predicts that the current is always carried by pairs of electrons in a spin singlet state, so conventional superconductivity decays very rapidly when in contact with a ferromagnet, which normally prohibits the existence of singlet pairs. It has been predicted that this rapid spatial decay would not occur when spin triplet superconductivity could be induced in the ferromagnet. Here we report a Josephson supercurrent through the strong ferromagnet CrO2, from which we infer that it is a spin triplet supercurrent. Our experimental setup is different from those envisaged in the earlier predictions, but we conclude that the underlying physical explanation for our result is a conversion from spin singlet to spin triplets at the interface. The supercurrent can be switched with the direction of the magnetization, analogous to spin valve transistors, and therefore could enable magnetization-controlled Josephson junctions.
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