Proximity effect in superconductor/conical magnet heterostructures
arXiv:1409.0366 · doi:10.1088/0953-8984/26/27/274212
Abstract
The presence of a spin-flip potential at the interface between a superconductor and a ferromagnetic metal allows for the generation of equal-spin spin-triplet Cooper pairs. These Cooper pairs are compatible with the exchange interaction within the ferromagnetic region and hence allow for the long-range proximity effect through a ferromagnet or half-metal. One suitable spin-flip potential is provided by incorporating the conical magnet Holmium (Ho) into the interface. The conical magnetic structure is characterised by an opening angle with respect to the crystal -axis and a turning (or pitch) angle measuring the rotation of magnetisation with respect to the adjacent layers. Here, we present results showing the influence of conical magnet interface layers with varying and on the efficiency of the generation of equal-spin spin-triplet pairing. The results are obtained by self-consistent solutions of the microscopic Bogoliubovde Gennes equations in the clean limit within a tight-binding model of the heterostructure. In particular, the dependence of unequal-spin and equal-spin spin-triplet pairing correlations on the conical magnetic angles and are discussed in detail.
12 pages, 6 figures
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Cited by in corpus (7)
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- Magnetoelectric Andreev effect due to proximity-induced non-unitary triplet superconductivity in helical metals
- Fulde-Ferrell-Larkin-Ovchinnikov state in spin-orbit-coupled superconductors
- Classification of magnetic inhomogeneities and transitions in superconducting-magnetic hybrid structures
- Spin-flipping with Holmium: Case study of proximity effect in superconductor/ferromagnet/superconductor heterostructures
- Influence of Magnetic Order on Proximity-Induced Superconductivity in Mn Layers on Nb(110) from First Principles
- Phase separation and proximity effects in itinerant ferromagnet-superconductor heterostructures