Proximity effects and triplet correlations in Ferromagnet/Ferromagnet/Superconductor nanostructures
arXiv:1207.1325 · doi:10.1103/PhysRevB.86.014523
Abstract
We report the results of a study of superconducting proximity effects in clean Ferromagnet/Ferromagnet/Superconductor () 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 as a function of the angle between the exchange fields in and . We find that the results for in systems are clearly different from those in systems, where monotonically increases with and is highest for antiparallel magnetizations. Here, is in general a non-monotonic function, and often has a minimum near . For certain values of the exchange field and layer thicknesses, the system exhibits reentrant superconductivity with : it transitions from superconducting to normal, and then returns to a superconducting state again with increasing . 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 . 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 . The local magnetization vector, which exhibits reverse proximity effects, is also investigated.
arXiv comment14 pages including 11 figures
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