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It is theoretically found that in-plane vortices may exist in a thin normal metal (N) layer (with thickness dN much smaller than the coherence length ξN) that covers a superconductor (S). Vortices enter the N layer with proximity-induced superconductivity at a sufficiently large in-plane magnetic field. These vorticies have squeezed cores and are located (pinned) near the SN interface. At large magnetic fields, we find a nascent vortex state, which is a spatially modulated state along the finite length N layer with zero vorticity. This state does not exist in a finite length single S layer.
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D. Yu. Vodolazov (2024) studied this question.
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