Superconductor Proximity Effect

When a normal metal (N) is placed in contact with a superconductor (S), Cooper pairs leak into N, inducing a spatially decaying superconducting gap Δ(x) ∝ e−x/ξ. This proximity effect is the basis for Andreev reflection and topological heterostructures.

1.00
0.60
0.90
Δ at x=ξ
Penetration depth
Interface Δ
Δ(x) = Δ₀ · T · exp(−x/ξ_N) for x > 0 (normal metal region)