Fig. 2

Dependence of the superconducting properties on the magnetic configuration. a Evolution of the local density of states (LDOS) as a function of the relative angle θ between the magnetisation of the ferromagnetic connector and the G^ϕ term of the S-node, showing zero-bias peaks with varying amplitude for parallel (θ = 0) and anti-parallel (θ = π) alignment and the appearance of the triplet gap around perpendicular alignment. b Pair amplitude of the mixed-spin and c, d the equal-spin components as a function of θ. The mixed-spin component is prominent for θ ≈ 0 and θ ≈ π and almost vanishes around θ = π/2, whereas for the equal-spin component it is opposite. All curves have been offset vertically for better visibility