Spin pumping between noncollinear ferromagnetic insulators through thin superconductors

TL;DR

This paper develops a theoretical framework using the generalized Usadel equation to analyze spin pumping between noncollinear ferromagnetic insulators through thin superconductors, revealing temperature-dependent spin current behaviors.

Contribution

It introduces a novel method to describe time-dependent spin transport in superconductor-ferromagnet systems and derives equations for spin currents considering noncollinear magnetizations.

Findings

Superconductors exhibit reduced spin accumulation compared to normal metals due to the energy gap.

The ratio of backflow spin currents in different magnetization configurations varies strongly with temperature.

The developed theory applies under conditions of sufficient dephasing and weak ferromagnetic polarization.

Abstract

Dynamical magnets can pump spin currents into superconductors. To understand such a phenomenon, we develop a method utilizing the generalized Usadel equation to describe time-dependent situations in superconductors in contact with dynamical ferromagnets. Our proof-of-concept theory is valid when there is sufficient dephasing at finite temperatures, and when the ferromagnetic insulators are weakly polarized. We derive the effective equation of motion for the Keldysh Green's function focusing on a thin film superconductor sandwiched between two noncollinear ferromagnetic insulators of which one is dynamical. In turn, we compute the spin currents in the system as a function of the temperature and the magnetizations' relative orientations. When the induced Zeeman splitting is weak, we find that the spin accumulation in the superconducting state is smaller than in the normal states due to the lack of quasiparticle states inside the gap. This feature gives a lower backflow spin current from the superconductor as compared to a normal metal. Furthermore, in superconductors, we find that the ratio between the backflow spin current in the parallel and anti-parallel magnetization configuration depends strongly on temperature, in contrast to the constant ratio in normal metals.