Induced Triplet Pairing in clean s-wave Superconductor/Ferromagnet layered structures

TL;DR

This paper investigates how triplet pairing correlations are induced in clean ferromagnet/superconductor/ferromagnet heterostructures, revealing long-range, time-dependent triplet correlations and local magnetization effects near interfaces.

Contribution

It provides a fully self-consistent numerical analysis of induced triplet correlations and magnetization phenomena in ferromagnet/superconductor layered structures with arbitrary magnetization angles.

Findings

Triplet correlations are induced alongside singlet correlations.

Triplet correlations are long-ranged and peak at inverse Debye frequency times.

Local magnetization oscillates and affects the density of states.

Abstract

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 $\alpha$ 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, 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, $\omega_D$, 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 $\alpha$.