Publication | Open Access
Induced triplet pairing in clean<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>s</mml:mi></mml:math>-wave superconductor/ferromagnet layered structures
83
Citations
27
References
2008
Year
Superconducting MaterialEngineeringLow-dimensional MagnetismMagnetic ResonanceOne-dimensional MagnetismMagnetic MaterialsSpin PhenomenonMagnetismInduced TripletSuperconductivityQuantum MaterialsTime-dependent Triplet CorrelationsMaterials ScienceQuantum ScienceHigh-tc SuperconductivityPhysicsCondensed Matter TheoryQuantum MagnetismNatural SciencesTriplet CorrelationsApplied PhysicsCondensed Matter Physics
We study induced triplet pairing correlations in clean ferromagnet/superconductor/ferromagnet heterostructures. The pairing state in the superconductor is the conventional singlet $s$ wave, and the angle $\ensuremath{\alpha}$ between the magnetizations of the two ferromagnetic layers is arbitrary. We use a numerical fully self-consistent solution of the microscopic equations and obtain the time-dependent triplet correlations via the Heisenberg equations of motion. We find that in addition to the usual singlet correlations, triplet correlations, which are odd in time as required by the Pauli principle, are induced in both the ferromagnets and the superconductor. These time-dependent correlations are largest at times of order of the inverse of the Debye cutoff frequency ${\ensuremath{\omega}}_{D}$, and we find that within that time scale, they are often spatially very long ranged. We discuss the behavior of the characteristic penetration lengths that describe these triplet correlations. We also find that the ferromagnets can locally magnetize the superconductor near the interface and that the local magnetization then undergoes strongly damped oscillations. The local density of states exhibits a variety of energy signatures, which we discuss, as a function of ferromagnetic strength and $\ensuremath{\alpha}$.
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