A1 Journal article (refereed)
Coexistence of superconductivity and spin-splitting fields in superconductor/ferromagnetic insulator bilayers of arbitrary thickness (2021)


Hijano, A., Ilić, S., Rouco, M., González-Orellana, C., Ilyn, M., Rogero, C., Virtanen, P., Heikkilä, T.T., Khorshidian, S., Spies, M., Ligato, N., Giazotto, F., Strambini, E., & Bergeret, F. S. (2021). Coexistence of superconductivity and spin-splitting fields in superconductor/ferromagnetic insulator bilayers of arbitrary thickness. Physical Review Research, 3(2), Article 023131. https://doi.org/10.1103/PhysRevResearch.3.023131


JYU authors or editors


Publication details

All authors or editors: Hijano, Alberto; Ilić, Stefan; Rouco, Mikel; González-Orellana, Carmen; Ilyn, Maxim; Rogero, Celia; Virtanen, P.; Heikkilä, T. T.; Khorshidian, S.; Spies, M.; et al.

Journal or series: Physical Review Research

eISSN: 2643-1564

Publication year: 2021

Publication date: 19/05/2021

Volume: 3

Issue number: 2

Article number: 023131

Publisher: American Physical Society (APS)

Publication country: United States

Publication language: English

DOI: https://doi.org/10.1103/PhysRevResearch.3.023131

Publication open access: Openly available

Publication channel open access: Open Access channel

Publication is parallel published (JYX): https://jyx.jyu.fi/handle/123456789/77101

Publication is parallel published: https://arxiv.org/abs/2012.15549


Abstract

Ferromagnetic insulators (FI) can induce a strong exchange field in an adjacent superconductor (S) via the magnetic proximity effect. This manifests as spin splitting of the BCS density of states of the superconductor, an important ingredient for numerous superconducting spintronics applications and the realization of Majorana fermions. A crucial parameter that determines the magnitude of the induced spin splitting in FI/S bilayers is the thickness of the S layer d: In very thin samples, the superconductivity is suppressed by the strong magnetism. By contrast, in very thick samples, the spin splitting is absent at distances away from the interface. In this work, we calculate the density of states and critical exchange field of FI/S bilayers of arbitrary thickness. From here, we determine the range of parameters of interest for applications, where the exchange field and superconductivity coexist. We show that for d>3.0ξs, the paramagnetic phase transition is always of the second order, in contrast to the first-order transition in thinner samples at low temperatures. Here ξs is the superconducting coherence length. Finally, we compare our theory with the tunneling spectroscopy measurements in several EuS/Al/AlOx/Al samples. If the Al film in contact with the EuS is thinner than a certain critical value, we do not observe superconductivity, whereas, in thicker samples, we find evidence of a first-order phase transition induced by an external field. The complete transition is preceded by a regime in which normal and superconducting regions coexist. We attribute this mixed phase to inhomogeneities of the Al film thickness and the presence of superparamagnetic grains at the EuS/Al interface with different switching fields. The steplike evolution of the tunnel-barrier magnetoresistance supports this assumption. Our results demonstrate on the one hand, the important role of the S layer thickness, which is particularly relevant for the fabrication of high-quality samples suitable for applications. On the other hand, the agreement between theory and experiment demonstrates the accuracy of our theory, which, originally developed for homogeneous situations, is generalized to highly inhomogeneous systems.


Keywords: superconductors; superconductivity; nanoelectronics


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Ministry reporting: Yes

Reporting Year: 2021

JUFO rating: 1


Last updated on 2022-20-09 at 14:32