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Proximity effects and triplet correlations in ferromagnet/ferromagnet/superconductor nanostructures

机译:铁磁体/铁磁体/超导体纳米结构中的邻近效应和三重态相关性

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We report the results of a study of superconducting proximity effects in clean ferromagnet/ferromagnet/ superconductor (F_1F_2S) heterostructures, where the pairing state in S is a conventional singlet s-wave. We numerically find the self-consistent solutions of the Bogoliubov-de Gennes (BdG) equations and use these solutions to calculate the relevant physical quantities. By linearizing the BdG equations, we obtain the superconducting transition temperatures T_c as a function of the angle α between the exchange fields in F_1 and F_2. We find (hat the results for T_c(α) in F_1F_2S systems are clearly different from those in F_1SF_2 systems, where T_c monotonically increases with α and is highest for antiparallel magnetizations. Here, T_c(α) is in general a nonmonotonic function, and often has a minimum near α≈80°. For certain values of the exchange field and layer thicknesses, the system exhibits reentrant superconductivity with α: it transitions from superconducting to normal, and then returns to a superconducting state again with increasing α. This phenomenon is substantiated by a calculation of the condensation energy. We compute, in addition to the ordinary singlet pair amplitude, the induced odd triplet pairing amplitudes. The results indicate a connection between equal-spin triplet pairing and the singlet pairing state that characterizes T_c. We find also that the induced triplet amplitudes can be very long ranged in both the S and F sides and characterize their range. We discuss the average density of states for both the magnetic and the S regions, and its relation to the pairing amplitudes and T_c. The local magnetization vector, which exhibits reverse proximity effects, is also investigated.
机译:我们报告了在干净的铁磁体/铁磁体/超导体(F_1F_2S)异质结构中超导邻近效应的研究结果,其中S中的配对状态是传统的单重态s波。我们在数值上找到Bogoliubov-de Gennes(BdG)方程的自洽解,并使用这些解来计算相关的物理量。通过线性化BdG方程,我们获得了超导转变温度T_c作为F_1和F_2中交换场之间的角度α的函数。我们发现(F_1F_2S系统中T_c(α)的结果与F_1SF_2系统中的T_c(α)的结果明显不同,T_c(α)的值随α单调增加,并且对于反平行磁化强度最高。这里,T_c(α)通常是非单调函数,并且通常在α≈80°附近有一个最小值,对于某些交换场和层厚度值,系统表现出具有α的折返超导性:它从超导过渡到法向,然后随着α的增加再次回到超导状态。通过冷凝能量的计算得到证实,除普通单线态对幅度外,还计算诱导的奇数三线态对幅度,结果表明等自旋三线态对与表征T_c的单线态对之间存在联系。还发现,诱导的三重态振幅在S和F侧都可以很长的距离分布并表征其范围,我们讨论了平均态密度对于磁性和S区域,它与配对幅度和T_c的关系。还研究了具有反向邻近效应的局部磁化矢量。

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